Trinocular stereo for non-parallel configurations
ITU-R BS.775-1 有无图像的多通道立体音响系统
RECOMMENDATION ITU-R BS.775-1*,**Multichannel stereophonic sound system withand without accompanying picture(1992-1994) The ITU Radiocommunication Assembly,consideringa) that it is widely recognized that a two-channel sound system has serious limitations and improved presentation is necessary;b) that the requirements of cinema presentation differ from those that apply in the home, particularly with respect to room and screen size and distribution of listeners, but that the same programmes may be reproduced in either the cinema or the home;c) that broadcast HDTV signals, and those delivered by other media, should be capable of giving appropriate sound quality with a wide range of domestic loudspeaker configurations, including compatibility with two-channel stereophonic and monophonic listening;d) that for multichannel sound it is desirable to separate the requirements of production, delivery and domestic presentation, though these are mutually interacting;e) that investigations about multichannel sound transmission and reproduction associated and not associated with accompanying picture are being carried out with the basic requirements as laid down in Annex 2;f) that one universal multichannel sound system applicable to both sound and television broadcasting would be beneficial to the listener;g) that compromises may be necessary to ensure that the system is as universal and as practical as possible;h) that a hierarchy of compatible sound systems for broadcasting, cinema and recordings is useful for programme exchange and up- and down-mixing depending on the programme material (see Annex 1);j) that ancillary services such as those for the visually impaired and hearing impaired are desirable;k) that advances in digital audio coding currently allow the delivery of multiple audio channels in an efficient manner,____________________*This Recommendation should be brought to the attention of the International Electrotechnical Commission (IEC) and the Society of Motion Picture and Television Engineers (SMPTE).** Radiocommunication Study Group 6 made editorial amendments to this Recommendation in 2002 in accordance with Resolution ITU-R 44.recommends1one universal multichannel stereophonic sound system, with or without accompanying picture, within a hierarchy given in Annex 1;2the following reference loudspeaker arrangement (see Fig. 1):–three front loudspeakers combined with two rear/side loudspeakers (Note 1);–the left and right frontal loudspeakers are placed at the extremities of an arc subtending 60︒at the reference listening point (Notes 2 and 3).Where for reasons of available space, it is preferred to place the frontal loudspeakers on a straight line base, then it may be necessary to introduce compensating time delays in the signal feed of the centre loudspeaker;–both side/rear loudspeakers should be placed within the sectors from 100︒ to 120︒ from the centre front reference. Precise location is not necessary. Side/rear loudspeakers should be no closer to the listener than the frontal loudspeakers, unless compensating time delay is introduced (Note 4);–the frontal loudspeakers should ideally be at a height approximately equal to that of the listener’s ears. This implies an acoustically transparent screen. Where a non-acoustically transparent screen is used, the centre loudspeaker should be placed immediately above or below the picture. The height of side/rear loudspeakers is less critical;3the use of five reference recording/transmission signals for left (L), right (R), centre (C), channels for the front, and left surround (LS) and right surround (RS) channels for the side/rear. Additionally the system may include a low frequency extension signal for a low frequency extension (LFE) channel (see Annex 7).In circumstances where transmission capacity or other constraints apply, the three front signals can be combined with one (mono surround, MS) or zero rear/side signals. In the case of mono surround, the MS signal is fed to both LS and RS loudspeakers (see Fig. 1);4compatibility, if required, with existing and low cost receivers by using one of the methods given in Annex 3;5down-mixing capability, if required, for reduction of the number of channels, either prior to transmission or at the receiver, by employing the down-mixing equations given in Table 2;6upward conversion where an increase in the number of channels is desired, either prior to transmission or at the receiver, by employing upwards-conversion techniques described in Annex 5; 7overall quality to the requirements of Annex 2;8provision (but see also § 9 below) for the following if necessary:–alternate multiple language principal services;–one or more independent channels carrying descriptive information for the visually impaired;–one or more independent channels for the purpose of supplying improved intelligibility to the hearing impaired;9additional data transmitted with the audio to enable the flexible use of the data capacity allocatable to audio signals (see Annex 6).D01FIGURE 1Reference loudspeaker arrangement withloudspeakers L/C/R and LS/RSLoudspeakerHorizontal angle fromcentre (degrees)Height (m)Inclination (degrees)C L, R LS, RS030100 (120)0 ... 15 down001.21.2≥ 1.2Screen 1 HDTV – Reference distance Screen 2H: height of screen B: loudspeaker base width = 3 H (2β = 33︒)= 2 H (2β = 48︒)12NOTE 1 – Optionally, there may be an even number of more than two rear/side loudspeakers which may provide a larger optimum listening area and greater envelopment.NOTE 2 – Optimum sound reproduction requires use of wide angular spacing between the left and right loudspeakers of two or three front loudspeaker channel stereophonic systems (see Fig. 1). It is recognized that the television pictures accompanying stereophonic sound having such an angular width cannot, with current techniques, be displayed to the same wide angles, but are often restrictedto 33︒horizontal subtended angle at the reference distance, although cinema images may be displayed at such angles (see Fig. 1). The resulting mismatch between picture and sound image width leads to differences in mixing technique for cinema and television. It is expected that larger television displays will lead to better compatibility of mixes for cinema and television display. NOTE 3 – The size of the loudspeaker basewidth, B (see Fig. 1), is defined for reference listening test conditions in Recommendation ITU-R BS.1116 –Methods for the subjective assessment of small impairments in audio systems including multichannel sound systems.NOTE 4 – If more than two rear/side loudspeakers are used, then the loudspeakers should be disposed symmetrically and at equal intervals on the arc which measures from 60︒ to 150︒ from the centre front reference (see Fig. 2).NOTE 5 – If more than two rear/side loudspeakers are used, the LS signal should be fed to each of the side/rear loudspeakers on the left side of the room and the RS signal should be fed to each of the side/rear loudspeakers on the right side of the room. In doing so, it will be necessary to reduce the signal gain such that the total power emitted by the loudspeakers carrying the LS (or RS) signal is the same as if that signal had been reproduced over a single loudspeaker. For large room reproduction, it may also be necessary to delay, or otherwise decorrelate, the feeds to some or all of the side/rear loudspeakers. Further studies on such decorrelation is necessary.FIGURE 2Optional 3/4 loudspeaker arrangement (3 front and 4 surround)ANNEX 1Hierarchy of compatible multichannel sound systemsfor broadcasting and recording(1)D03 In the case of mono surround the signal feeding LS and RS should preferably be decorrelated.ANNEX 2Basic requirementsThe following requirements are related to the specified multichannel sound system with and without accompanying picture.1The directional stability of the frontal sound image shall be maintained within reasonable limits over a listening area larger than that provided by conventional two-channel stereophony.2The sensation of spatial reality (ambience) shall be significantly enhanced over that provided by conventional two-channel stereophony. This shall be achieved by the use of side and/or rear loudspeakers.3It is not required that the side/rear loudspeakers should be capable of the prescribed image locations outside the range of the front loudspeakers.4Downward compatibility with sound systems providing lower number of channels (down to stereophonic and monophonic sound systems) shall be maintained (see Annex 1).5Real-time mixing for live broadcast shall be practicable.6In cases where the number of delivered signals is smaller than the number of reproduction channels upward conversion should be ensured to an acceptable degree (see Annex 5).7The basic audio quality of the sound reproduced after decoding must be subjectively indistinguishable from the reference for most types of audio programme material. Using the triple stimuli with hidden reference test implies grades consistently higher than four on the ITU-R impairment 5-grade scale. The most critical material must not be graded lower than four.8For the objective quality parameters Recommendations ITU-R BS.644 and ITU-R BS.645 shall be the basis, superseded by new measuring methods for digital techniques. (These matters are under study by the ITU-R.)9Listening test conditions are currently under study in the ITU-R.10For subjective assessments see Recommendation ITU-R BS.1116.11The synchronization of sound and vision signals are currently under study in the ITU-R.12Optimum economy shall be pursued in all respects, including both cost and transmission bandwidth.ANNEX 3Compatibility1 Backward compatibility with existing receiversIn the case that an existing 2/0 channel format is extended to a 3/2 channel format, two methods have been identified to assure backward compatibility with existing receivers.One method is to continue providing the existing 2/0 channel service and to add the new 3/2 channel service. This approach is referred to as a simulcasting operation. The advantage of this approach is that the existing 2/0 service could be discontinued at some point in the future. Another method is the use of compatibility matrices. The matrix equations shown in Table 1 may be used to provide compatibility with existing receivers. In this case, the existing Left and Right emission channels are used to convey the compatible A and B matrix signals. Additional emission channels are used to convey the T, Q1, and Q2 matrix signals. The advantage of this approach is that less additional data capacity is required to add the new service.TABLE 1Five channel surround: encoding and decoding equations2 Downward compatibility with low-cost receiversTwo methods have been identified which provide downward compatibility with low receiver complexity. The first requires the use of the matrix process described in § 1. A low-cost receiver then only requires the A- and B-channels as in the case of the 2/0 system i.e. a system which does not use a backwards compatibility matrix.The second method is applicable to the discrete 3/2 delivery system. The delivered signals are digitally combined using the equations in Annex 4, which enable the required number of signals to be provided. In the case of low bit-rate source coded signals, the downward mixing of the 3/2 signals may be performed prior to the synthesis portion of the decoding process (where the bulk of the complexity lies).ANNEX 4Downward mixing of multichannel audio signals1 3/2 source signalsTable 2 shows a set of equations that may be used to mix the five signals of the 3/2 system down to the formats: 1/0; 2/0; 3/0; 2/1; 3/1; 2/2.TABLE 2Downward mixing equations for 3/2 source materialIt should be noted that the overall effect of such downward mixing equations (and compatibility matrixing, see Annex 3) will depend on other factors, such as the panning equations and microphone characteristics. It is recommended that further studies on such interactions be carried out (see Annex 8).ANNEX 5Upwards conversionUpwards conversion is needed in cases where the number of production channels is smaller than the number of channels available for reproduction. A typical example is a 2-channel stereo programme (2/0) that is to be presented over a 3/2 reproduction system.Upwards conversion involves the generation of the “missing” channels somewhere in the broadcast chain. When performing upwards conversion, the following guidelines should normally be respected in order that the programme makers have a reference arrangement. These guidelines do not exclude the possibility, for receiver manufacturers, of the implementation of more sophisticated techniques.1 Frontal channels1.1When a monophonic programme is to be presented over a reproduction system with three frontal loudspeakers, the mono signal should be presented over the centre loudspeaker only. When two frontal loudspeakers are only available, the mono signal should be presented over both left and right loudspeakers with an attenuation of 3 dB.1.2When a stereophonic programme is to be presented over a reproduction system with three frontal loudspeakers, the left and right signals of the stereo programme should be presented respectively over the left and right loudspeakers only.2 Surround channels2.1When there is no surround signal in a programme, surround loudspeakers should not be activated.2.2When a given surround signal is to be reproduced over more than one loudspeaker, decorrelation between each loudspeaker signal should be performed. Furthermore, proper attenuation should be applied to each loudspeaker signal so that the combined sound pressure level produced by these loudspeakers should match that of a single frontal loudspeaker if fed by the same signal at a given reference listening position.3 Data channelAuxiliary information describing the mode of transmission (number and type of transmitted channels) should be transmitted periodically in a special data channel in parallel with the programme. This information will be needed to perform upwards conversion in receivers.ANNEX 6Additional data*It is necessary that some additional data are sent to the multichannel sound receiver, to enable it to identify the multichannel sound configuration in use, and provide the loudspeakers with the required signals. Implicit in the ability to reconfigure a multichannel sound system is the ability to use the available sound channels flexibly, so that a wide range of applications can be covered.The details of the additional data (bit rate, data format, etc.) have yet to be determined. However, the following applications, which would need to be signalled in the data channel, have been identified:–the signalling and controlling of different multichannel sound configurations for the main programme and conversion (e.g. 5-channel, 3-channel, 2-channel, mono) to other configurations;–indicating a special sound signal for listeners with impaired hearing;–indicating a special sound signal for viewers with impaired sight;–indicating a separate audio programme (SAP);____________________*Further studies and contributions from administrations are necessary.–conveying dynamic range control information, to compress or expand the dynamic range; –conveying characters for a text service;–flexible usage of the data capacity allocated for audio signals.ANNEX 7Subwoofer channel or low frequency extension channel (LFE)The purpose of this optional channel is to enable listeners, who choose to, to extend the low frequency content of the reproduced programme in terms of both frequency and level. In this way it is the same as the subwoofer channel proposed by the film industry for their digital sound systems. In the film industry the subwoofer channel carries high level, low frequency sound effects which are intended to be fed to (a) specific low frequency loudspeaker(s). In that way the magnitude of the low frequency content of the other channels is restricted so that the main loudspeakers are not required to handle these special effects signals. The main film sound channels carry normal low frequency sounds but not at such high levels. They are therefore sufficient on their own if these special effects are not required by the user. This combination has the other benefit that the coding of the high level signals in the subwoofer channel can be optimized without affecting the coding of the main channels.Although it is recognized that the number of domestic consumers who will choose to use a subwoofer channel is likely to be restricted, it is also recognized that there are other future applications of the HDTV sound system under discussion that will make more use of this option, e.g. distribution of signals to cinemas.The subwoofer channel should not, however, be used for the entire low frequency content of the multi-channel sound presentation. The subwoofer channel is an option, at the receiver, and thus should only carry the additional enhancement information.(In a similar way, the surround channels should carry their own low frequency information rather than it being mixed into the front channels. This forward mixing of the low frequency sounds is an option, at the receiver, to decrease the requirements on the surround loudspeakers.)The subwoofer channel should be capable of handling signals in the range 20-120 Hz.The level at which the subwoofer channel should be reproduced, relative to the main channels, is still to be studied. It is noted, however, that the film industry is currently coding the subwoofer channel such that a positive gain of 10-12 dB is required on reproduction. A common standard on this point will obviously be beneficial.The coding of the main channels should not place any reliance on masking provided by the subwoofer channel. The coding of the subwoofer channel may, however, assume masking due to sounds reproduced from the main channels.ANNEX 8Compatibility matrixing and downward mixingMethods for providing backward compatibility and downward compatibility are described in Annex 3. Annex 4 contains downward mixing equations for 3/2 source material.However, it is recognized that the alternative down-mix coefficients for the surround signals LS/RS are desirable, depending on the type of the programme material.Four alternative surround signal down-mix coefficients should be indicated by the broadcaster.0.70710.50000.0000ReservedAdditional data should be transmitted to indicate which coefficient should be used.。
显微镜学术语(一)
Microscope GlossaryBelow you will find explanations for many of the common words used in microscopy. Abbe Condenser: A specially designed lens that mounts under the stage and is usually movable in the vertical direction. It has an iris type aperture to control the diameter of the beam of light entering the lens system. By changing the size of the iris and moving the lens toward or away from the stage, the diameter and focal point of the cone of light that goes through the specimen can be controlled. Abbe condensers really become useful at magnifications above400X. The condenser lens system should have a numerical aperture equal to or greater than the N.A. of the objective lens being used. All of our microscopes that go to 1000X use Abbe condensers with a 1.25 N.A. There are twotypes. One is a spiral type that you turn to move it up or down and the other is on a rack and pinion system and controlled with a condenser focusing knob. Achromatic lenses: When light goes through a prism or lens, it is bent or refracted. Some colors refract more than others and as a result, will focus at different points, reducing resolution. To help correct this problem, achromatic lenses are used. These lenses are made of different types of glass with different indexes of refraction. The result is a better (but not perfect) alignment of some of the colors at the focal point, thereby giving you a clearer image.Arm: The part of the microscope that connects the tube to the base. When carrying a microscope, grab the arm with one hand and place your other hand under the base.Articulated Arm: A type of stand that holds a microscope body. The stand clamps to a table and has a variety of motion in three dimensions.Base: The bottom support of the microscope (see arm above).Binocular Head: A microscope head with two eyepiece lenses, one for each eye. Generally this term is used in describing a high power (compound) microscope. With a low power microscope we say "stereo" head because, unlike the compound microscope, the stereo has a separate objective lens for each eyepeice lens, producing two independent paths of light, one for each eye. In the compound microscope with a binocular head, there are two eyepiece lenses but still only one objective lens and you will not get stereo vision.Body: This term is used mostly with the low power stereo microscopes and it is the basic heart of the microscope without any type of stand (base) or illuminators. It usually includes the eyepiece and objective lenses but not the focusing block.C-mount: This is an adapter used with various types of video cameras. Usually, you unscrew the lens from the camera and screw in the adapter. The adapterthen connects to the trinocular port on the microscope.Coarse Focus: This is the rough focus knob on the microscope. You use it to move the objective lenses toward or away from the specimen (see fine focus).Coaxial Focus: A focusing system that has both the coarse and fine focusing knobs mounted on the same axis. Usually the coarse knob is larger and on the outside and the fine knob is smaller and on the inside. On some coaxial systems, the fine adjustment is calibrated, allowing differential measurements to be recorded.Condenser Lens: A lens mounted in or below the stage whose purpose is to focus or condense the light onto the specimen. The higher power objective lenses have very tiny diameters and require concentrated light to work properly. By using a condenser lens you will increase the Illumination and resolution. Condenser lenses are not required on low power microscopes. Contrast Plate: A circular opaque plate placed on the stage of a low power microscope. One side is white, the other is black. It can be flipped around depending on the coloration of your specimen.Cover Slip: A very thin square piece of glass or plastic placed over the specimen on a microscope slide. When used with liquid samples, it flattens out the liquid and assists with single plane focusing.Diaphragm: Generally a five hole disc placed under the stage on a high power microscope. Each hole is of a different diameter. By turning it, you can vary the amount of light passing through the stage opening. This will help to properly illuminate the specimen and increase contrast and resolution. The diaphragm is most useful at the higher powers.DIN Optics: A German standard for the manufacturing of microscopelenses. DIN lenses aren't particularly better than non-DIN but they will be interchangeable from one DIN microscope to another. They are set to work with a 160mm tube length and have a uniform thread. Most quality microscopes use DIN optics.Diopter Adjustment: When you look through a microscope with two eyepiece lenses, you must be able to change the focus on one eyepiece to compensate for the difference in vision between your two eyes. The diopter adjustment does this. The way to correctly adjust this is to first close the eye over the eyepiece with the diopter adjustment and normally focus the microscope so that the open eye sees the image in focus. Next, switch eyes (close the open eye, open the closed eye) and without changing the main focus knobs, focus on the image by turning the diopter adjustment only. Now with both eyes open, the image should be clear with both eyes. (This technique is used with binoculars too.)Dual Head: A microscope (usually high power) with a single eyepiece lens coming out one side and an additional single eyepiece tube coming either off thetop or from the opposite side. Dual heads are used so that a teacher can verify what a student is seeing or can be used for video or camera work. It is not recommended that two students do a lab sharing a single dual microscope as it will get to be uncomfortable for the student using the top eyepiece.Eyepiece Lens: The lens at the top of the microscope that you look into. They are usually 10X but also are available in 5X, 15X and 20X. Widefield lenses have a large diameter and show a wide area of the field of view.Fine Focus: This is the knob used to fine tune the focus on the specimen. It is also used to focus on various parts of the specimen. Generally one uses the coarse focus first to get close then moves to the fine focus knob for fine tuning.Field of View: Sometimes abbreviated "FOV", it is the diameter of the circle of light that you see when looking into a microscope. As the power gets greater, the field of view gets smaller. You can measure this by placing a clear metric ruler on the stage and counting the millimeters from one side to the other. Typically you will see about 4.5mm at 40X, 1.8mm at 100X, 0.45mm at 400X and 0.18mm at 1000X. See micrometer.Fixed Arm: A type of stand used with low power microscopes. The arm and body are integral parts of the microscope and connected solidly to the base.Focus: A means of moving the specimen closer or further away from the objective lens to render a sharp image. On some microscopes, the stage moves and on others, the tube moves. Rack and pinion focusing is the most popular and durable type.Head: The upper part of the microscope that contains the eyepiece tube and prisms. A monocular head has one eyepiece, a binocular has two (one for each eye), a dual head has two but they are not together, and a trinocular head has three, one which is generally used for a camera connection.Illuminator: A light source mounted under the stage. Three types of light are commonly used: Tungsten, Fluorescent and Halogen. Tungsten is the least expensive and most common. Fluorescent is bright, white and runs cool and Halogen is very bright and white but gives off heat like tungsten.Immersion Oil: A special oil used in microscopy with only the 100X objective lens (usually at 1000X total power). A drop is placed upon the cover slip and the objective is lowered until it just touches the drop. Once brought into focus, the oil acts as a bridge between the glass slide and the glass in the lens. This concentrates the light path and increasing the resolution of the image. Both Type A and Type B are commonly used in light microscopy and the only difference is the viscosity (B is more viscous).Inclination Joint: Where the arm connects to the base, there may be a pin. If so, you can place one hand on the base and with the other grab the arm and rotate it back. It will tilt your microscope back for more comfortable viewing. Onedrawback of tilting it back is that wet samples will run off the slide.Interpupiliary Adjustment (also called Inter Ocular Distance I.O.D.): When using a stereo or binocular microscope there must be an adjustment for the distance between the viewer’s eyes. A young child will have a small interpupiliary distance and an adult a larger one. The eyepiece lenses will spread apart or get closer together to fit each individual. This should be the first adjustment to make so that you are comfortably viewing the specimen with both eyes.Mechanical Stage: A mechanical way to move the slide around on your stage. It consists of a slide holder and two knobs. Turn one knob and the slide moves toward or away from you. Turn the other knob and the slide moves left and right. Since everything is upside down on a (high power) microscope it takes some getting used to but it is very convenient to have one especially when observing moving specimens like protozoans or other pond watercritters. Microscopes either have the bolt on mechanical stage that can be added (to many models) at any time or the integral mechanical stage that comes built in to the microscope.Micrometer: Also called a micron it is the metric linear measurement used in microscopy. There are 1000 microns in a millimeter. If something is 1.8mm long then it can also be expressed as 1,800 microns (or micrometers) long.Mirror: Allows you to direct ambient light up through the hole in the stage and illuminate the specimen.Monocular Head: A microscope head with a single eyepiece lens.Nosepiece: The part of the microscope that holds the objective lenses also called a revolving nosepiece or turret.Numerical Aperture (N.A.): This is a number that expresses the ability of a lens to resolve fine detail in an object being observed. It is derived by a complex mathematical formula and is related to the angular aperture of the lens and the index of refraction of the medium found between the lens and the specimen. To get the best possible image, you should have a condenser system that matches or exceeds the N.A. of the highest power objective lens on yourmicroscope. (note, N.A. is only important with high power microscopes).Objective Lens: The lens closest to the object. In a stereo (low power) microscope there are objective pairs, one lens for each eyepiece lens. This gives the 3-D effect. On a high power binocular model there is still only one objective lens so no stereo vision.Oil Immersion Lens: An objective lens (usually 100X or greater) designed to work with a drop of special oil placed between it and the slide. With oil, an increase in resolution will be noticed. Also, see "Immersion Oil" above.Parcentered: This is an alignment issue. When changing from one objective lens to another, the image of the object should stay centered. Test this by centering something in your field of view. Change to a higher power. Is it still centered? Almost all microscopes are parcentered.Parfocal: This is a focus issue. When changing from one objective to another, the new image should be either in focus or close enough so that you can refocus with only minor adjustments. Most microscopes are parfocal.Pointer: When you look through the eyepiece lens, you may see a pointer. By turning the eyepiece, you can rotate the pointer around.Post Stand: A type of stand used with low power microscopes. It consists of a single post rising vertically from the base. The microscope body can rotate about the post and also be moved up and down on it.Rack and Pinion: The rack is a track with teeth and the pinion is a gear that rides on the teeth. By turning a knob, the pinion gear moves along therack. These systems are used in focusing mechanisms, in Abbe condenser focusing systems, and on mechanical stages to move the slide around.Rack Stop (or Safety Rack Stop): Usually set at the factory, the rack stop keeps you from cranking the objective lenses too far down (damaging something). If you are using a very thin slide, you may find that you can't get the high power objective lens close enough to the slide to focus. Here you can either adjust the rack stop or place a thin glass slide under your original slide, making it closer to the lens.Resolution: The ability of a lens system to show fine details of the object being observed.Reticle: A very tiny grid pattern inserted in an eyepiece lens. It is used to make actual measurements of the size of objects seen through the microscope. Revolving Nosepiece: See nosepieceRing Light: An independent light that usually connects to the microscope body and gives off a ring of light.Semi-Plan Lenses: Lenses are never perfect. If you were looking at something perfectly flat, you might find that much of the center part of your field of view is in focus but out on the edges it is fuzzy and a bit out of focus. Semi-plan lenses improve this deficiency by showing sharper images and less aberrations in the perimeter of the field of view. They are better than standard achromatic lenses but cost quite a bit more.Slide: A flat glass or plastic rectangular plate that the specimen is placed on. It may have a depression or well to hold a few drops of liquid.Slip Clutch: When students bring the focus all the way up or down and continue to try turning the knob, damage to the focusing system can occur if there wasn't a slip clutch. It is a mechanical device that protects the gears of the microscope.Stage: The flat plate where the slides are placed for observation.Stage Clips: Clips on the stage used to hold the slide in place.Stage Plate: On a low power microscope, there is a frosted circular glass plate that fits in over the lower illuminator. This is called the stage plate. See also contrast plate.Stand: On a low power microscope, the type of connection between the microscope body and the base. There are three main types: the post, the fixed arm and the universal boom stand.Stereo: Related to microscopes, seeing with both eyes through separate eyepiece and objective lenses. With two objectives, the image looks 3-D, we see it in "stereo"! See also Binocular head.Student Proofed: We're always trying to outwit the students. Many of the classroom type microscopes have just about everything locked down. You need special tools to remove eyepiece lenses, objective lenses and they have all the safety devices like the rack stop. Not totally student proofed (like drop proof!) but close.Sub-stage: The area below the stage as in "sub stage illuminator"T-mount: A type of adapter used to mate still cameras (usually 35mm) to microscopesTension Adjustment: This is an adjustment of the focusing mechanism that is made at the factory. It is set so that the instrument is easy to focus but also tight enough so that the stage doesn't drift when you are not focusing. Stage drift is caused by the weight of the stage (or tube) automatically unfocusing the microscope.Trinocular Head: Available on both high and low power microscopes, tri heads have two eyepiece lenses (one for each eye) and a third port at the top for a camera. Some microscopes give you the option of sending all the light to the tri port, or perhaps half and half, or maybe 70/30%. On some stereo tri heads with dual power, the tri port transmits the image through the set of lenses not being used by the stereo eyepieces.Turret: See nosepiece.Universal Stand: A long boom type arm used to support a (low power) microscope body. It has many adjustments allowing the microscope to be aligned in a wide variety of configurations. Generally one uses an external (like afiber optic) light source with a universal stand.Widefield eyepiece lenses: These are wide diameter glass eyepiecelenses. They offer the greatest field of view when looking at specimens.X: Times as in 200X or two hundred times magnification. The magnification of a microscope is determined by multiplying the power of the eyepiece lens by the power of the corresponding objective lens.XR: The X is times (see above) and the R stands for retractable. These objective lenses have a spring loaded tip so if they hit the slide, they will retract, and telescope inward. This prevents damage to the lens or slide。
EMF EMT EMTR EMX系列双目显微镜使用说明书
EMF EMT EMTR EMX S eriesINSTRUCTIONMANUAL2 - 34445 - 755667777 - 8788999910-13NOMENCLATURE AND FUNCTION THE USE AND CARE UnpackingHow to Rotate the Head OPERATION PROCEDURES How To Operate Illuminators Focusing Capability Precise Focus On Specimen Focusing ProcedureInterpupillary Distance AdjustmentChanging The Magnification On EMT, EMTR And EMX Models How To Use EyeshieldPHOTOGRAPHY AND TELEVISION Photography Camera Operation TelevisionMAINTENANCE AND CARE Bulb Replacement Care CleaningEM Series SYSTEM DIAGRAM12MEIJI EMF EMT EMTR EMX Series STEREO MICROSCOPEPhoto TubePilar CollarDimmer Switch (PBH Stand)Prism HouseTurret ObjectiveIncident Illuminator Lamp CoverStage Clips Glass Stage PlateBase with Transformer and Transmitted Illuminator built inSelector Switch (I)(T)(IT)Incident Light Incident ands to the film planeModel EMT-1 with SWF10X mounted on PBH (PB) StandEMTR-2Trinocular Stereo Body Eyetube Inclination : 45Adjustment Ring3Set screwEyeshieldClampCollar Set ScrewBaseEyepieceswith EyeshieldPrism HouseFixed objectiveStage ClipsStage Plate Set ScrewReversible Stage Plate Black / WhiteModel EMF-1 with SWF10X mounted on P StandModel EMX-1 with SWF10Xmounted on PX StandThe MEIJI EM Series (EMF,EMT, EMTR and EMX Series) Widefield Stereo Microscope consists of two converging compound microscopes which are combined as a unit to focus simultaneously on the same field of object. Each body tube is fitted with a set of Porro prisms to erect the image and matchedachromatic objectives and super widefield eyepieces to furnish a very wide flat field of view. Each eye observes the object from a different perspective, consequently, deep stereoscopic relief is produced in the fused image.This MEIJI EM Series Stereo Microscope widely is used for various applications such as assembly and inspection of semiconductor devices, and as an indispensable part in bonding machines and microtomes, as well as for educational, clinical and research purposes.This series stereo microscope is used as follows:UNPACKINGThis EM series stereo microscope is usually supplied in a styrofoam containers. Remove theinstrument from its container by grasping the stereo microscope body and supporting the base with the other hand.Place the instrument on a firm flat table. (No packing material should be discarded until the instrument has been checked, since some may contain accessory equipment which can not be attached to the instrument.)When supplied in a wooden cabinet, remove the instrument from the cabinet by unscrewing the two large screws which are used to fasten the instrument to the cabinet through the bottom of the cabinet, with a coin or large screwdriver.If you ordered zoom stereo body and stand separately, loosen the set screw and insert the body into the holder then tighten the set screw after setting at the desired position.How to Rotate the Head:A special feature of this series stereo microscope is the rotation of the stereo microscope body through 360 so that it can be utilized either in the conventionalposition or with the stage nearest to the observer. To rotate the stereo microscope body, loosen the set screw.4THE USE AND CARE OFMEIJI EM SeriesWIDEFIELD STEREO MICROSCOPEInsert the eyepieces into eyetubeon the holder5IMPORTANT!Before plugging the illuminator into any electric outlet, make sure that transfomers and illumination bases supplied to you are suitable to the current available. (When shipped, these will be labelled as to mains voltage and cycles specification.)FOCUSING CAPABILITYThe Pole-type focusing stands have a double focusing capability, i.e. Rough Focus (by sliding the whole focus assembly and stereo body up and down on the pillar, fixing the clamp screw when in approximate focus on yourspecimen), Precise Focus (by using the rack and pinion focusing knob).The focusing stands, P , PL, PX, PC, PB, PBH and BX are the Pole-type.Before moving the whole focus assembly up and down for rough focus, loosen pillar collar once and make sure to reset after the rough focusing is done.How to use selector switch and dimmer switchFocusing stands, PBH, ABH and ABE, are using 6V 10W Halogen lamps with suitabletransformers built-in base and a selector switch and a dimmer switch on the base.Select an illuminator to use, either incident or transmitted, by the selector switch in the way described above. Then, turn the dimmer switch knob slowly to clockwise to turn the dimmer switch ON and to increase brightness. Turn the knob to counterclockwise to decrease the brightness and to turn OFF.Focusing assemblyHOW TO OPERATE ILLUMINATORSHow to use selector switchFocusing stands, PB and AB, are using 6V 1.2A (7W) tungsten filament bulb with suitabletransformer built-in base and selector switch on the base.Turn the selector switch knob to indicate I for oblique illumination, to indicate T for transmitted illumination and IT for simultaneous illumination by oblique and transmitted lights. The selector switch has OFF position at the both right and left ends.OPERATION PROCEDURESPB StandDimmer Switch6The Rigid arm type focusing stands (except the model ABE) have a focusing capability only by rack and pinion adjustment. This means that the available range of specimen sizes/depths which can be accommodated is somewhat less than in the case of Pole-type stands.The Rigid arm type ABE focusing stand is with integral focus block and extendable working distance. Provides transmitted and incident halogen illumination.set the screw back.A, AB and ABH stands are rigid arm type focusing stands.AB StandAB StandABE Extendable StandLook through the right eyepiece and, using only the right eye, focus on a plain surfaced objectivecentered on the stage. Adjust the focusing knob until the image is sharp without disturbing the focusing knob.Look through the left eyepiece and, using only the left eye, adjust the Eyepiece Adjusting Ring, clockwise or counterclockwise, until the image is in sharp focus.Each observer must focus the microscope to his individual requirements. However, a change of specimen requires only a slight readjustment of the focus.(1)(2)(3)An alternate scheme for focusing may be used. Instead of closing either eye, the left or right side can be blocked off by holding a bit of opaque material below one side or the other of the eyepiece, and the same basic procedure followed as above.Focusing ProcedureWhen replacing stage plate loosen the set screw which is visible in front of the stage.PRECISE FOCUS ON SPECIMENStage PlatesYou should now decide which of the stage plates supplied will be most suitable.The focusing stands with plain bases, P , PL, PX, PC and A, are supplied with reversible black and white stage plates. Your selection depends on which side, black or white, gives the best contrast conditions with your selected specimen.The focusing stands with transmitted illuminators, PB, PBH, AB, ABH and ABE, are supplied with clear glass stage plates and reversible black and white stage plates. If the specimen is semi-transparent, the glass stage plate shoud be used with transmitted illumination switched on. If the specimen is opaque, use the black/white stage. Your selection depends on which side, black and white, gives the best contrast.7Interpupillary Distance Adjustment:The distance between the eyepiece tubes can be adjusted to the proper interpupillary distance of the observer. Take the both sides of Prism Houses in your hands and move inward and outward, looking through theeyepieces, until the both fields are viewed asFused."Fused"Changing the Magnification on EMT, EMTR and EMX ModelsThe EMT, EMTR and EMX models have the paired objectives in a rotatable mount for rapid selection ofmagnification. To change the magnification, hold the knurled part of the objective cover and rotate clockwise or counterclockwise until it clicks and stop.How to Use EyeshieldEyeshields which slip over Super Widefield Eyepieces are supplied. These eyeshields exclude stray light and orient the eyes in the proper relationship to the eyepieces.DiopterPHOTOGRAPHYPhotographic documentation of microscope visual images is most conveniently achieved by using the trinocular (photo-binocular) bodies offered for use with MEIJI TECHNO microscpoes.In the case of the EMTR Stereo series a trinocular is supplied with lever-switching of the image from one of the binocular eyepieces vertically up to the film plane of a 35mm SLR camera with adaptor mounted on the vertical photo tube. Visual observation can be simultaneously carried out, using the other eyepiece.In this system the MA150/50 and MA150/60 Camera Attachment should be used with the SLR camera model of your choice. Please note that one of the large range of T2 Adaptor Rings suiting to your camera should have been ordered and supplied.These adaptor rings are intended to compensate for the small differences in effective distance of the film plane in your camera - so as to ensure that photographs are optimally sharp, and achieved without wastage of film in trial shots and experimentation.In addition special low-power camera eyepieces (2.5X, 3.3X and 5X) are available and recommended - these will give you maximum field coverage on your specimen while using the convenient and economical 35mm film formatPHOTOGRAPHY AND TELEVISION54-74mm8TELEVISIONFor television the MA 151/5N "C" Mount Adaptor should be used, threaded into your TV camera, then placed and adjusted on the upper portion of your trinocular body.Adjustment can then proceed a per paragraph (3) above. You should understand that thecomparatively large magnification factors inherent in most TV camera/monitor systems will restrict your fields of view (while blowing up total magnification).A correct optical set-up and adjustment is, of course, crucial to obtaining a good TV monitor image, but keep in mind that the monitor controls for brightness and contrast adjustment are also important and should also be experimented with in order to obtain the best monitor image.CAMERA OPERATION(1)(2)(3)or MA150/60 Camera Attachment, thenthe trinocular body.Pull out the lever on your trinocular body so as to send the image both to the camera and the visual eyepiece.Rotate the adjustment ring on the straight tube so as to set the red indicator line on the You now should be set correctly for optimum and photography.CK3900N or CK3900PMK300N or MK300P CK3900N or CK3900P MK300N or MK300P *35mm SLR9BULB REPLACEMENTWhen changing light bulbs in the illuminators, always disconnect the plug from the electrical source. Never work on the electrical system without first disconnecting.When a bulb replacement is necessary in the Incident Illuminator, remove the lamp cover by turning it counterclockwise and remove the old bulb by twisting it 1/3 turn counterclockwise by pushing it toward the socket so that the bulb will be sprung out from its socket.To replace the bulb of the Transmitted Illuminator, lay the instrument carefully over on its side and remove the four set screws in the bottom cover of the base. Replace the old bulb in the same way as above.The bulbs used for the Incident and Transmitted Illuminators of PB/AB stand are different. The bulb for the Incident Illuminator employs a flat filament facing to the head of the bulb and Catalog Number is MA560 and the bulb for the Transmitted Illuminator employs a flat filament facing to the side of the lamp and the Catalog Number is MA561. The bulbs used for the Incident and Transmitted Illuminators of PBH/ABH/ABE stand are same halogen. Catalog number is MA570.CAREAlways cover the instrument with the plastic dust cover provided when the microscope is not in use.Keep the eyepieces in the microscope body at all times in order to prevent dust from falling on the internal optics.Store the microscope in a safe, clean place when not in use for an extended period of time.CLEANINGClean exposed lens surfaces carefully with a pressurized air source, soft brush or clean soft cloth.Too much finger pressure may damage lens coatings.To remove oil fingerprints and grease smudges, moisten the cleaning cloth with a very small amount of alcohol or xylene.Painted or plastic surfaces should be cleaned only with a cloth moistened with water and a small amount of detergent.DO NOT ATTEMPT TO MAKE ADJUSTMENTS TO THE INTERNAL OPTICS OR MECHANICS!!If the microscope does not seem to be functioning properly or you have questions about its operation, call your supplier (or an authorized repair service) for advice.MAINTENANCE AND CARESet screw in rubber footBottom cover plateTurn to unscrewFor Transmitted lightFor Both lightFor Incident lightPBAB StandsPBH ABHABE Stands26mmIncident bulb replacement26mm25mmMA560MA561MA570EM Series SYSTEM DIAGRAM SPECIAL STANDSEMF-1, EMF-2,EMT-1, EMT-2, EMT-3, EMT-4,EMTR-1, EMTR-2, EMTR-3, EMTR-4,S-4100w/400mm Pole S-4200w/610mm PoleS-4300w/400mm Pole S-4400w/610mm PoleS-4500w/400mm PoleFX Holderw/illuminator portFS Holderw/illuminator port for bonding machineFC Holderw/coaxial coares and fine focusing blockF HolderFX Holderw/illuminator portFC Holderw/coaxial coares and fine focusing blockF HolderSBUUniversal Stand ULUniversal Stand MUUniversal StandMA574Large Sliding StageMA575Medium Sliding StageMA574Large Sliding StageMA575Medium Sliding StageFA-1Articulated Arm Stand FA-2Articulated Arm StandEM Series VIEWING HEADS10EMZ-1, EMZ-2, EMZ-5, EMZ-5D, EMZ-6, EMZ-9,EMZ-10, Z-7100, EMZ-2TR, EMZ-5TR, EMZ-5TRD, EMZ-8TR, EMZ-8TRDZOOM HEADS :EMF-1, EMF-2,EMT-1, EMT-2, EMT-3, EMT-4,EMTR-1, EMTR-2, EMTR-3, EMTR-4,EM Series VIEWING HEADSEMZ-1, EMZ-2, EMZ-5, EMZ-5D,EMZ-6, EMZ-9, EMZ-10, Z-7100, EMZ-2TR, EMZ-5TR, EMZ-5TRD, EMZ-8TR, EMZ-8TRDZOOM HEADS :CK3900N or CK3900PMK300N or MK300P CK3900N or CK3900P MK300N or MK300P EM Series SYSTEM DIAGRAMEM Series SYSTEM DIAGRAMMA565Ungraduated mechanical stageMA564Graduated mechanical stageMA550/05MA565/05Ungraduated mechanical stagewith clear glass plate(Polarizer)with clear glass plate12MA667Polarizing Plate (Polarizer)KBL Pole type w/illuminater port on flat baseKBE Rigid-extendable arm on flat baseMA551Extension poleMA569Clear glass stage plateMA569Clear glass stage plateMA569Clear glass stage plateMA569Clear glass stage plateMA567Acrylic frosted stage plate MA567Acrylic frosted stage plate MA567Acrylic frosted stage plate MA567Acrylic frosted stage plate MA551Extension pole AB Rigid-arm w/tungsten 6V 7W trans/incident lights ABH Rigid-arm w/halogen 6V 10W trans/incident lights ABE Extendable w/halogen 6V 10W trans/incident lights BX Stand w/mirror for B/D(light not included)B mirror Stand 115V 20W MA537Protective glassMA658Protective glassMA6520.7XMA550/10Polarizing filter (Analyzer)MA564/05Graduated mechanical stagewith clear glass plate MA565/05Ungraduated mechanical stagewith clear glass plateMA5180.5XMA5270.75XMA5131.5XMA5142.0XAuxiliary lensesAuxiliary lensEMT-3EMTR-3EMT-4EMTR-4EMX*MA501SWF5XMA502SWF10XMA520SWF12.5XMA503SWF15XMA535HSWF15XMA504SWF20XMA521SWF30XMA519*SWF10X-F *(Piece)MA600EYESHIELDEYEPIECES, Paired*Need to use PX stand or Pole type stand with MA551 Extension pole.132186 Bering Drive San Jose, CA., 95131, USAE-mail:*********************Phone : 408-428-9654 Fax : 408-428-0472Toll free : 800-832-0060322-1,Chikumazawa Miyoshi-machi, Iruma-gunSaitama 354-0043, Japan E-mail:********************.jpPhone : (0)49-259-0111 Fax : (0)49-259-011303.10.2,000 V1 Printed in Japan。
高中英语 精华双语文章 四类作曲家素材
高中精华双语文章:四类作曲家音乐史上众多的作曲家,根据其创作方式的不同,可分为四大类:自发式灵感型、建设型、传统类及先锋型。
跟着文章了解一下舒伯特、贝多芬等著名作曲家们各属于什么类型吧。
The Four Types of Composers四类作曲家I can see three different types of composers in musical history, each of whom creates music in a somewhat different fashion.我发现音乐史上有三种不同类型的作曲家,他们各自创作的方式有不同。
The type that has fired public imagination most is that of the spontaneously inspired composer - the Franz Schubert type, in other words. All composers are inspired, of course, but this type is more spontaneously inspired. Music simply wells out of him. He can't get it down on paper fast enough. You can almost tell this type of composer by his fruitful output. In certain months, Schubert wrote a song a day. Hugo Wolf did the same.最能激发公众想象力的是自发式灵感型即弗朗兹·舒伯特型。
当然所有的作曲家都需要灵感,但这一类型的更具自发的灵感,音乐简直就是喷涌而出,多得来不及记录,通过他们多产的作品你几乎可以一下就认出他们。
人工智能AI革命外文翻译中英文
人工智能(AI)革命外文翻译中英文英文The forthcoming Artificial Intelligence (AI) revolution:Its impact on society and firmsSpyros MakridakisAbstractThe impact of the industrial and digital (information) revolutions has, undoubtedly, been substantial on practically all aspects of our society, life, firms and employment. Will the forthcoming AI revolution produce similar, far-reaching effects? By examining analogous inventions of the industrial, digital and AI revolutions, this article claims that the latter is on target and that it would bring extensive changes that will also affect all aspects of our society and life. In addition, its impact on firms and employment will be considerable, resulting in richly interconnected organizations with decision making based on th e analysis and exploitation of “big” data and intensified, global competition among firms. People will be capable of buying goods and obtaining services from anywhere in the world using the Internet, and exploiting the unlimited, additional benefits that will open through the widespread usage of AI inventions. The paper concludes that significant competitive advantages will continue to accrue to those utilizing the Internet widely and willing to take entrepreneurial risks in order to turn innovative products/services into worldwide commercial success stories. The greatest challenge facing societies and firms would be utilizing the benefits of availing AI technologies, providing vast opportunities for both new products/services and immense productivity improvements while avoiding the dangers and disadvantages in terms of increased unemployment and greater wealth inequalities.Keywords:Artificial Intelligence (AI),Industrial revolution,Digital revolution,AI revolution,Impact of AI revolution,Benefits and dangers of AI technologies The rise of powerful AI will be either the best or the worst thing ever to happento humanity. We do not yet know which.Stephen HawkingOver the past decade, numerous predictions have been made about the forthcoming Artificial Intelligence (AI) Revolution and its impact on all aspects of our society, firms and life in general. This paper considers such predictions and compares them to those of the industrial and digital ones. A similar paper was written by this author and published in this journal in 1995, envisioning the forthcoming changes being brought by the digital (information) revolution, developing steadily at that time, and predicting its impact for the year 2015 (Makridakis, 1995). The current paper evaluates these 1995 predictions and their impact identifying hits and misses with the purpose of focusing on the new ones being brought by the AI revolution. It must be emphasized that the stakes of correctly predicting the impact of the AI revolution arefar reaching as intelligent machines may become our “final invention” that may end human supremacy (Barrat, 2013). There is little doubt that AI holds enormous potential as computers and robots will probably achieve, or come close to, human intelligence over the next twenty years becoming a serious competitor to all the jobs currently performed by humans and for the first time raising doubt over the end of human supremacy.This paper is organized into four parts. It first overviews the predictions made in the 1995 paper for the year 2015, identifying successes and failures and concluding that major technological developments (notably the Internet and smartphones) were undervalued while the general trend leading up to them was predicted correctly. Second, it investigates existing and forthcoming technological advances in the field of AI and the ability of computers/machines to acquire real intelligence. Moreover, it summarizes prevailing, major views of how AI may revolutionize practically everything and its impact on the future of humanity. The third section sums up the impact of the AI revolution and describes the four major scenarios being advocated, as well as what could be done to avoid the possible negative consequences of AI technologies. The fourth section discusses how firms will be affected by these technologies that will transform the competitive landscape, how start-up firms are founded and the way success can be achieved. Finally, there is a brief concluding section speculating about the future of AI and its impact on our society, life, firms and employment.1. The 1995 paper: hits and missesThe 1995 paper (Makridakis, 1995) was written at a time when the digital (at that time it was called information) revolution was progressing at a steady rate. The paper predicted that by 2015 “the information revolution should be in full swing” and that “computers/communications” would be in widespread use, whi ch has actually happened, although its two most important inventions (the Internet and smartphones) and their significant influence were not foreseen as such. Moreover, the paper predicted that “a single computer (but not a smartphone) can, in addition to its traditional tasks, also become a terminal capable of being used interactively for the following:” (p. 804–805)• Picture phone and teleconference• Television and videos• Music• Shopping• On line banking and financial services• Reservations• Medic al advice• Access to all types of services• Video games• Other games (e.g., gambling, chess etc.)• News, sports and weather reports• Access to data banksThe above have all materialized and can indeed be accessed by computer,although the extent of their utilization was underestimated as smartphones are now being used widely. For instance, the ease of accessing and downloading scientific articles on one's computer in his/her office or home would have seemed like science fiction back in 1995, when finding such articles required spending many hours in the library (often in its basement for older publications) and making photocopies to keep them for later use. Moreover, having access, from one's smartphone or tablet, to news from anywhere in the world, being able to subscribe to digital services, obtain weather forecasts, purchase games, watch movies, make payments using smartphones and a plethora of other, useful applications was greatly underestimated, while the extensive use of the cloud for storing large amounts of data for free was not predicted at all at that time. Even in 1995 when the implications of Moore's law leading to increasing computer speed and storage while reducing costs were well known, nevertheless, it was hard to imagine that in 2016 there would be 60 trillion web pages, 2.5 billion smartphones, more than 2 billion personal computers and 3.5 billion Google searches a day.The paper correctly predicted “as wireless telecommunications will be possible the above list of capabilities can be accessed from anywhere in the world without the need for regular telephone lines”. What the 1995 paper missed, however, was that in 2015 top smartphones, costing less than €500, would be as powerful as the 1995 supercomputer, allowing access to the Internet and all tasks that were only performed by expensive computers at that time, including an almost unlimited availability of new, powerful apps providing a large array of innovative services that were not imagined twenty years ago. Furthermore, the paper correctly predicted super automation leading to unattended factories stating that “by 2015 there will be little need for people to do repetitive manual or mental tasks”. It also foresaw the decline of large industrial firms, increased global competition and the drop in the percentage of labour force employed in agriculture and manufacturing (more on these predictions in the section The Impact of the AI Revolution on Firms). It missed however the widespread utilization of the Internet (at that time it was a text only service), as well as search engines (notably Google), social networking sites(notably Facebook) and the fundamental changes being brought by the widespread use of Apple's iPhone, Samsung's Galaxy and Google's Android smartphones. It is indeed surprising today to see groups of people in a coffee shop or restaurant using their smartphones instead of speaking to each other and young children as little as three or four years of age playing with phones and tablets. Smartphones and tablets connected to the Internet through Wi-Fi have influenced social interactions to a significant extent, as well as the way we search for information, use maps and GPS for finding locations, and make payments. These technologies were not predicted in the 1995 paper.2. Towards the AI revolutionThe 1995 paper referred to Say, the famous French economist, who wrote in 1828 about the possibility of cars as substitutes for horses:“Nevertheless no machine will ever be able to perform what even the worst horses can - the service of carrying people and goods through the bustle and throng of a great city.” (p. 800)Say could never have dreamed of, in his wildest imagination, self-driving cars, pilotless airplanes, Skype calls, super computers, smartphones or intelligent robots. Technologies that seemed like pure science fiction less than 190 years ago are available today and some like self-driving vehicles will in all likelihood be in widespread use within the next twenty years. The challenge is to realistically predict forthcoming AI technologies without falling into the same short-sighted trap of Say and others, including my 1995 paper, unable to realize the momentous, non-linear advancements of new technologies. There are two observations to be made.First, 190 years is a brief period by historical standards and during this period we went from horses being the major source of transportation to self-driving cars and from the abacus and slide rules to powerful computers in our pockets. Secondly, the length of time between technological inventions and their practical, widespread use is constantly being reduced. For instance, it took more than 200 years from the time Newcomen developed the first workable steam engine in 1707 to when Henry Ford built a reliable and affordable car in 1908. It took more than 90 years between the time electricity was introduced and its extensive use by firms to substantially improve factory productivity. It took twenty years, however, between ENIAC, the first computer, and IBM's 360 system that was mass produced and was affordable by smaller business firms while it took only ten years between 1973 when Dr Martin Cooper made the first mobile call from a handheld device and its public launch by Motorola. The biggest and most rapid progress, however, took place with smartphones which first appeared in 2002 and saw a stellar growth with the release of new versions possessing substantial improvements every one or two years by the likes of Apple, Samsung and several Chinese firms. Smartphones, in addition to their technical features, now incorporate artificial intelligence characteristics that include understanding speech, providing customized advice in spoken language, completing words when writing a text and several other functions requiring embedded AI, provided by a pocket computer smaller in size than a pack of cigarettes.From smart machines to clever computers and to Artificial Intelligence (AI) programs: A thermostat is a simple mechanical device exhibiting some primitive but extremely valuable type of intelligence by keeping temperatures constant at some desired, pre-set level. Computers are also clever as they can be instructed to make extremely complicated decisions taking into account a large number of factors and selection criteria, but like thermostats such decisions are pre-programmed and based on logic, if-then rules and decision trees that produce the exact same results, as long as the input instructions are alike. The major advantage of computers is their lightning speed that allows them to perform billions of instructions per second. AI, on the other hand, goes a step further by not simply applying pre-programmed decisions, but instead exhibiting some learning capabilities.The story of the Watson computer beating Jeopardy's two most successful contestants is more complicated, since retrieving the most appropriate answer out of the 200 million pages of information stored in its memory is not a sign of real intelligence as it relied on its lightning speed to retrieve information in seconds. What is more challenging according to Jennings, one of Jeopardy's previous champions, is“to read clues in a natural language, understand puns and the red herrings, to unpack just the meaning of the clue” (May, 2013). Similarly, it is a sign of intelligence to improve it s performance by “playing 100 games against past winners”. (Best, 2016). Watson went several steps beyond Deep Blue towards AI by being able to understand spoken English and learn from his mistakes (New Yorker, 2016). However, he was still short of AlphaGo that defeated Go Champions in a game that cannot be won simply by using “brute force” as the number of moves in this game is infinite, requiring the program to use learning algorithms that can improve its performance as it plays more and more gamesComputers and real learning: According to its proponents, “the main focus of AI research is in teaching computers to think for themselves and improvise solutions to common problems” (Clark, 2015). But many doubt that computers can learn to think for themselves even though they can display signs of intelligence. David Silver, an AI scientist working at DeepMind, explained that “even though AlphaGo has affectively rediscovered the most subtle concepts of Go, its knowledge is implicit. The computer parse out these concepts –they simply emerge from its statistical comparisons of types of winning board positions at GO” (Chouard, 2016). At the same time Cho Hyeyeon, one of the strongest Go players in Korea commented that “AlphaGo seems like it knows everything!” while others believe that “AlphaGo is likely to start a ‘new revolution’ in the way we play Go”as “it is seeking simply to maximize its probability of reaching winning positions, rather than as human players tend to do –maximize territorial gains” (Chouard, 2016). Does it matter, as Silver said, that AlphaGo's knowledge of the game is implicit as long as it can beat the best players? A more serious issue is whether or not AlphaGo's ability to win games with fixed rules can extend to real life settings where not only the rules are not fixed, but they can change with time, or from one situation to another.From digital computers to AI tools: The Intel Pentium microprocessor, introduced in 1993, incorporated graphics and music capabilities and opened computers up to a large number of affordable applications extending beyond just data processing. Such technologies signalled the beginning of a new era that now includes intelligent personal assistants understanding and answering natural languages, robots able to see and perform an array of intelligent functions, self-driving vehicles and a host of other capabilities which were until then an exclusive human ability. The tech optimists ascertain that in less than 25 years computers went from just manipulating 0 and 1 digits, to utilizing sophisticated neural networkalgorithms that enable vision and the understanding and speaking of natural languages among others. Technology optimists therefore maintain there is little doubt that in the next twenty years, accelerated AI technological progress will lead to a breakthrough, based on deep learning that imitates the way young children learn, rather than the laborious instructions by tailor-made programs aimed for specific applications and based on logic, if-then rules and decision trees (Parloff, 2016).For instance, DeepMind is based on a neural program utilizing deep learning that teaches itself how to play dozens of Atari games, such as Breakout, as well or better than humans, without specific instructions for doing so, but by playing thousands ofgames and improving itself each time. This program, trained in a different way, became the AlphaGo that defeated GO champion Lee Sodol in 2016. Moreover, it will form the core of a new project to learn to play Starcraft, a complicated game based on both long term strategy as well as quick tactical decisions to stay ahead of an opponent, which DeepMind plans to be its next target for advancing deep learning (Kahn, 2016). Deep learning is an area that seems to be at the forefront of research and funding efforts to improve AI, as its successes have sparked a burst of activity in equity funding that reached an all-time high of more than $1 billion with 121 projects for start-ups in the second quarter of 2016, compared to 21 in the equivalent quarter of 2011 (Parloff, 2016).Google had two deep learning projects underway in 2012. Today it is pursuing more than 1000, according to their spokesperson, in all its major product sectors, including search, Android, Gmail, translation, maps, YouTube, and self-driving cars (The Week, 2016). IBM's Watson system used AI, but not deep learning, when it beat the two Jeopardy champions in 2011. Now though, almost all of Watson's 30 component services have been augmented by deep learning. Venture capitalists, who did not even know what deep learning was five years ago, today are wary of start-ups that do not incorporate it into their programs. We are now living in an age when it has become mandatory for people building sophisticated software applications to avoid click through menus by incorporating natural-language processing tapping deep learning (Parloff, 2016).How far can deep learning go? There are no limits according to technology optimists for three reasons. First as progress is available to practically everyone to utilize through Open Source software, researchers will concentrate their efforts on new, more powerful algorithms leading to cumulative learning. Secondly, deep learning algorithms will be capable of remembering what they have learned and apply it in similar, but different situations (Kirkpatrick et al., 2017). Lastly and equally important, in the future intelligent computer programs will be capable of writing new programs themselves, initially perhaps not so sophisticated ones, but improving with time as learning will be incorporated to be part of their abilities. Kurzweil (2005) sees nonbiological intelligence to match the range and subtlety of human intelligence within a quarter of a century and what he calls “Singularity” to occur by 2045, b ringing “the dawning of a new civilization that will enable us to transcend our biological limitations and amplify our creativity. In this new world, there will be no clear distinction between human and machine, real reality and virtual reality”.For some people these predictions are startling, with far-reaching implications should they come true. In the next section, four scenarios associated with the AI revolution are presented and their impact on our societies, life work and firms is discussed.3. The four AI scenariosUntil rather recently, famines, wars and pandemics were common, affecting sizable segments of the population, causing misery and devastation as well as a large number of deaths. The industrial revolution considerably increased the standards of living while the digital one maintained such rise and also shifted employment patterns,resulting in more interesting and comfortable office jobs. The AI revolution is promising even greater improvements in productivity and further expansion in wealth. Today more and more people, at least in developed countries, die from overeating rather than famine, commit suicide instead of being killed by soldiers, terrorists and criminals combined and die from old age rather than infectious disease (Harari, 2016). Table 1 shows the power of each revolution with the industrial one aiming at routine manual tasks, the digital doing so to routine mental ones and AI aiming at substituting, supplementing and/or amplifying practically all tasks performed by humans. The cri tical question is: “what will the role of humans be at a time when computers and robots could perform as well or better andmuch cheaper, practically all tasks that humans do at present?” There are four scenarios attempting to answer this question.The Optimists: Kurzweil and other optimists predict a “science fiction”, utopian future with Genetics, Nanotechnology and Robotics (GNR) revolutionizing everything, allowing humans to harness the speed, memory capacities and knowledge sharing ability of computers and our brain being directly connected to the cloud. Genetics would enable changing our genes to avoid disease and slow down, or even reverse ageing, thus extending our life span considerably and perhaps eventually achieving immortality. Nanotechnology, using 3D printers, would enable us to create virtually any physical product from information and inexpensive materials bringing an unlimited creation of wealth. Finally, robots would be doing all the actual work, leaving humans with the choice of spending their time performing activities of their choice and working, when they want, at jobs that interest them.The Pessimists: In a much quoted article from Wired magazine in 2000, Bill Joy (Joy, 2000) wrote “Our most powerful 21st-century technologies –robotics, genetic engineering, and nanotech –are threatening to make humans an endangered species”. Joy pointed out that as machines become more and more intelligent and as societal problems become more and more complex, people will let machines make all the important decisions for them as these decisions will bring better results than those made by humans. This situation will, eventually, result in machines being in effective control of all important decisions with people dependent on them and afraid to make their own choices. Joy and many other scientists (Cellan-Jones, 2014) and philosophers (Bostrom, 2014) believe that Kurzweil and his supporters vastly underestimate the magnitude of the challenge and the potential dangers which can arise from thinking machines and intelligent robots. They point out that in the utopian world of abundance, where all work will be done by machines and robots, humans may be reduced to second rate status (some saying the equivalent of computer pets) as smarter than them computers and robots will be available in large numbers and people will not be motivated to work, leaving computers/robots to be in charge of making all important decisions. It may not be a bad world, but it will definitely be a different one with people delegated to second rate status.Harari is the newest arrival to the ranks of pessimists. His recent book (Harari, 2016, p. 397) concludes with the following three statements:• “Science is converging to an all-encompassing dogma, which says thatorganisms are algorithm s, and life is data processing”• “Intelligence is decoupling from consciousness”• “Non-conscious but highly intelligent algorithms may soon know us better than we know ourselves”Consequently, he asks three key questions (which are actually answered by the above three statements) with terrifying implications for the future of humanity: • “Are organisms really just algorithms, and is life just data processing?”• “What is more valuable –intelligence or consciousness?”• “What will happen to society, polit ics and daily life when non-conscious but highly intelligent algorithms know us better than we know ourselves?”Harari admits that nobody really knows how technology will evolve or what its impact will be. Instead he discusses the implications of each of his three questions: • If indeed organisms are algorithms then thinking machines utilizing more efficient ones than those by humans will have an advantage. Moreover, if life is just data processing then there is no way to compete with computers that can consult/exploit practically all available information to base their decisions.• The non-conscious algorithms Google search is based on the consultation of millions of possible entries and often surprise us by their correct recommendations. The implications that similar, more advanced algorithms than those utilized by Google search will be developed (bearing in mind Google search is less than twenty years old) in the future and be able to access all available information from complete data bases are far reachi ng and will “provide us with better information than we could expect to find ourselves”.• Humans are proud of their consciousness, but does it matter that self-driving vehicles do not have one, but still make better decisions than human drivers, as can be confirmed by their significantly lower number of traffic accidents?When AI technologies are further advanced and self-driving vehicles are in widespread use, there may come a time that legislation may be passed forbidding or restricting human driving, even though that may still be some time away according to some scientists (Gomes, 2014). Clearly, self-driving vehicles do not exceed speed limits, do not drive under the influence of alcohol or drugs, do not get tired, do not get distracted by talking on the phone or sending SMS or emails and in general make fewer mistakes than human drivers, causing fewer accidents. There are two implications if humans are not allowed to drive. First, there will be a huge labour displacement for the 3.5 million unionized truck drivers in the USA and the 600 thousand ones in the UK (plus the additional number of non-unionized ones) as well as the more than one million taxi and Uber drivers in these two countries. Second, and more importantly, it will take away our freedom of driving, admitting that computers are superior to us. Once such an admission is accepted there will be no limits to letting computers also make a great number of other decisions, like being in charge of nuclear plants, setting public policies or deciding on optimal economic strategies as their biggest advantage is their objectivity and their ability to make fewer mistakes than humans.One can go as far as suggesting letting computers choose Presidents/PrimeMinisters and elected officials using objective criteria rather than having people voting emotionally and believing the unrealistic promises that candidates make. Although such a suggestion will never be accepted, at least not in the near future, it has its merits since people often choose the wrong candidate and later regret their choice after finding out that pre-election promises were not only broken, but they were even reversed. Critics say if computers do eventually become in charge of making all important decisions there will be little left for people to do as they will be demoted to simply observing the decisions made by computers, the same way as being a passenger in a car driven by a computer, not allowed to take control out of the fear of causing an accident. As mentioned before, this could lead to humans eventually becoming computers’ pets.The pragmatists: At present the vast majority of views about the future implications of AI are negative, concerned with its potential dystopian consequences (Elon Musk, the CEO of Tesla, says it is like “summoning the demon” and calls the consequences worse than what nuclear weapons can do). There are fewer optimists and only a couple of pragmatists like Sam Altman and Michio Kaku (Peckham, 2016) who believe that AI technologies can be controlled through “OpenAI” and effective regulation. The ranks of pragmatists also includes John Markoff (Markoff, 2016) who pointed out that the AI field can be distinguished by two categories: The first trying to duplicate human intelligence and the second to augment it by expanding human abilities exploiting the power of computers in order to augment human decision making. Pragmatists mention chess playing where the present world champion is neither a human nor a computer but rather humans using laptop computers (Baraniuk, 2015). Their view is that we could learn to exploit the power of computers to augment our own skills and always stay a step ahead of AI, or at least not be at a disadvantage. The pragmatists also believe that in the worst of cases a chip can be placed in all thinking machines/robots to render them inoperative in case of any danger. By concentrating research efforts on intelligence augmentation, they claim we can avoid or minimize the possible danger of AI while providing the means to stay ahead in the race against thinking machines and smart robots.The doubters: The doubters do not believe that AI is possible and that it will ever become a threat to humanity. Dreyfus (1972), its major proponent, argues that human intelligence and expertise cannot be replicated and captured in formal rules. He believes that AI is a fad promoted by the computer industry. He points out to the many predictions that did not materialize such as those made by Herbert A. Simon in 1958 that “a computer would be the world's chess champion within ten years” and those made in 1965 that “machines will be capable within twenty years, of doing any work a man can do” (Crevier, 1993). Dreyfus claims that Simon's optimism was totally unwarranted as they were based on false assumptions that human intelligence is based on an information processing viewpoint as our mind is nothing like a computer. Although, the doubters’ criticisms may have been valid in the last century, they cannot stand for the new developments in AI. Deep Blue became the world's chess champion in 1997 (missing Simon's forecast by twenty one years) while we are not far today from machines being capable of doing all the work that humans can do (missing。
基于有序图像的快速三维重建
基于有序图像的快速三维重建刘保江;尹颜朋【摘要】如何提高重建速度一直是三维重建中的一个关键问题.传统的三维重建方法由于需要对输入的所有图像做任意两图像之间的匹配,故不适合大场景的重建.提出一种基于有序图像的快速三维重建方法,仅需对有序图像序列中的相邻图像做匹配,减少匹配阶段时间,从而提高重建速度.实验结果表明,提出的方法与传统的全匹配方法相比,能达到相同水平的重建效果,但在重建速度上具有明显的优势.【期刊名称】《现代计算机(专业版)》【年(卷),期】2017(000)035【总页数】4页(P81-84)【关键词】三维重建;SFM;快速重建【作者】刘保江;尹颜朋【作者单位】四川大学计算机学院,成都 610065;四川大学计算机学院,成都610065【正文语种】中文0 引言计算机三维重建技术是当前研究的一个热点。
三维重建目的是从输入的多张二维场景图像恢复出场景三维立体模型。
与传统的利用激光扫描仪等精密设备直接测量出物体三维模型相比具有方便、成本低以及适用范围广等优点,在文物考古、医疗卫生、旅游、数字娱乐和军事测绘导航等各个领域应用广泛。
进几十年来出现了许多基于图像视觉的三维重建方法,例如明暗度法[1-3]、纹理法[4-6]、轮廓法[7-8]、运动法[9]、调焦法[10]、双目视觉法[11]和多目视觉法[12]等。
但是大都存在重建精度较差、鲁棒性较差问题,或是重建效果不错,但存在运算时间太长问题。
故如何在达到不错的重建质量基础上提高重建速度就显得十分重要。
针对上面提出的方法存在的问题,本文提出一种基于有序图像序列的快速三维重建方法,在三维重建过程中,仅对相邻的图像进行特征匹配,对于n张输入图像,能够将匹配阶段的时间复杂度从O(n2)降低到O(n),对于大场景的重建在时间上节省尤为明显。
然后利用多视图几何和对极几何约束关系,计算出场景的几何结构和摄像机的参数信息,重建出场景的三维立体模型,并使重建质量达到传统的三维重建的水平。
3d设备
一.Quantel 3D制作系统的功能1.iQ: online finishing and DI at SD, HD, 2K, 4K and Stereo3D2.Pablo: grading and finishing for HD, 2K, 4K and Stereo3DAdditionally all existing Pablo 4K or iQ systems can upgrade to Stereoscopic 3D, providing a 'start to finish' Stereo workflow including previsualisation, editing, VFX, colour correction, trailers and mastering.——2007参与作品《阿凡达》3.Sid: Stereo3D workstationEnterprise sQ complete Stereo3D workflowQuantel's world-leading Enterprise sQ server based production system supports Stereo3D content right through the pipeline from ingest to desktop editing and craft editing to playout. This development delivers the same great Quantel Enterprise sQ workflow that is relied on by so many broadcasters around the world, but now for the first time working with Stereo3D content.Stereo3D RecordingsQ Server ingests Stereo3D (left eye and right eye)as Stereo clips under the control of the sQ Recordapplication. Stereo clips are recorded in DVCPROHD using 100 Mbit for each eye. An H.264 browsecopy is created simultaneously to allow frameaccurate editing using desktop editors.Stereo3D input ports can be configured to automatically invert or reverse either eye from a mirror rig, saving time by removing the need to manually flip the image in an editor.The clip will appear in the server bin as a Stereo clip - complete with a new stereo icon. Stereo clips and conventional clips can co-exist on the same server.Stereo3D Desktop EditingsQ View and sQ Cut provide low cost shot selection and simple editing tools. As both left and right eye browse is created by the sQ, operators can monitor each eye to check for mismatches.Stereo3D Craft EditingA new Stereo3D craft editor is available to provide acomprehensive toolset for manipulating 3D. Thecraft editor supports side-by-side, top-and-bottomand line-interleave multiplexing modes. It alsosupports checkerboard and flicker display modesfor even more Stereo3D flexibility.Stereo3D OutputThe sQ server can play out separate left and righteye channels or multiplex them together onto asingle HDSDI stream.Complete Enterprise sQ Stereo3D Workflow (asshown at NAB 2010)二.3d的拍摄设备1.垂直支架上下垂直的立体拍摄架适合拍摄距离较近的图像,因为上下垂直方式的3D立体拍摄架能够将两台机器的夹角调节到较小的范围,更接近人眼的程度。
W (P, t)=
ON THE CHARNEY-DAVIS AND NEGGERS-STANLEYCONJECTURESVICTOR REINER AND VOLKMAR WELKERAbstract.For a graded naturally labelled poset P,it is shownthat the P-Eulerian polynomialW(P,t):= w∈L(P)t des(w)counting linear extensions of P by their number of descents hassymmetric and unimodal coefficient sequence,verifying the moti-vating consequence of the Neggers-Stanley conjecture on real zeroesfor W(P,t)in these cases.The result is deduced from McMullen’sg-Theorem,by exhibiting a simplicial polytopal sphere whose h-polynomial is W(P,t).Whenever this simplicial sphere turns out to beflag,that is,its minimal non-faces all have cardinality two,it is shown that theNeggers-Stanley Conjecture would imply the Charney-Davis Con-jecture for this sphere.In particular,it is shown that the sphereisflag whenever the poset P has width at most2.In this case,the sphere is shown to have a stronger geometric property(locallyconvexity),which then implies the Charney-Davis Conjecture inthis case via a result from[30].It is speculated that the proper context in which to view both of these conjectures may be the theory of Koszul algebras,and someevidence is presented.1.IntroductionThis paper has several goals.Thefirst is to show that,in the context of the Neggers-Stanley Conjecture1.2,for every graded poset P there is lurking in the background a polytopal simplicial sphere,which we will denote∆eq(P).This sphere is relevant for two purposes:2VICTOR REINER AND VOLKMAR WELKER⊲The P-Eulerian polynomial(defined below)coincides with theh-polynomial of∆eq(P).As a consequence,its coefficients sat-isfy McMullen’s conditions for the h-vector of a simplicial poly-tope,and are in particular symmetric and unimodal.Therebywe verify the motivating consequence of the Neggers-StanleyConjecture for naturally labeled graded posets(see discussionafter the statement of Conjecture1.2).⊲Whenever the simplicial sphere∆eq(P)isflag,the Neggers-Stanley Conjecture1.2for P implies the Charney-Davis Con-jecture for the sphere∆eq(P).Furthermore,when P has widthat most2,it is shown in Theorem3.23that∆eq(P)satisfies astronger geometric condition thanflag-ness known as local con-vexity,which implies the Charney-Davis Conjecture in this caseby a result from[30].The latter portion of the paper(Section4onward)is aimed toward the thesis that both the Charney-Davis and Neggers-Stanley Conjec-tures,along with some other combinatorial conjectures and results, should be considered in the context of the following question. Question1.1.For which Koszul algebras is the Hilbert function a Polya frequency sequence?To give a more precise discussion,we start by recalling the Neggers-Stanley Conjecture.For any partial order P on[n]:={1,2,...,n}, let L(P)denote its set of linear extensions,that is the set of w= (w1,...,w n)∈S n for which i<P j implies w−1(i)<w−1(j).The P-Eulerian polynomialW(P,t):= w∈L(P)t des(w)is the generating function for the linear extensions L(P)counted ac-cording to cardinality of their descent sets:Des(w):={i∈[n−1]:w i>w i+1}des(w):=#Des(w)Conjecture1.2(Neggers-Stanley).For any labelled poset P on[n] the polynomial W(P,t)has only real(non-positive)zeroes.We are mainly interested in the case where P is naturally labelled, that is i<P j implies i<j.Some history and context for the conjecture follows.For naturally labelled posets Conjecture1.2was made originally by Neggers[32], and generalized to the above statement by Stanley in1986.When P is an antichain of n elements,W(P,t)is the Eulerian polynomial whoseCHARNEY-DAVIS AND NEGGERS-STANLEY CONJECTURES3 real-rootedness was shown by Harper[24]and served as an initial mo-tivation for the conjecture.For the case when P is a naturally labelled disjoint union of chains the result is due to Simion[37].This result was extended to arbitrary labellings by Brenti[7],who also verified the conjecture for Ferrers posets and Gaussian posets[7].An impor-tant combinatorial implication of the real-rootedness of a polynomial with non-negative coefficients is the unimodality of the coefficients(i.e. for the sequence of coefficients a0,...,a r there is an index j such that a0≤···≤a j≥···≥a r).Gasharov[19]verified the unimodality consequence of the conjecture for naturally labelled graded posets with at most3ranks.Corollary3.15verifies this(and something stronger) more generally for all naturally labelled graded posets.Next,we recall the Charney-Davis Conjecture.Given an abstract simplicial complex∆triangulating a(d−1)-dimensional(homology) sphere,one can collate the face numbers f i,which count the number of i-dimensional faces,into its f-vector and f-polynomialf(∆):=(f−1,f0,f1,...,f d−1)f(∆,t):=d i=0f i−1t i.The h-polynomial and h-vector are easily seen to encode the same in-formation:(1.1)h(∆):=(h0,h1,...,h d)whereh(∆,t)=di=0h i t i satisfies t d h(∆,t−1)= t d f(∆,t−1) t→t−1.The h-polynomial turns out to be a more convenient and natural encoding in several ways,closely related to commutative algebra,toric geometry,and shellability.For example,the fact that homology spheres are Cohen-Macaulay implies non-negativity of the h i,and the Dehn-Sommerville equations for simplicial spheres assert that h i=h d−i for 0≤i≤d(see[46,§II.6]).Note that the latter implies that the h-polynomial is symmetric,h(∆,t)=t d h(∆,t−1),and that h(∆,−1)=0 whenever d is odd.The Charney-Davis Conjecture[11,Conjecture D]concerns the quan-tity h(∆,−1)in the case where d is even and∆is a simplicial homology (d−1)-sphere which happens to be aflag complex,that is the minimal subsets of vertices which do not span a simplex all have cardinality4VICTOR REINER AND VOLKMAR WELKERtwo.For polytopal simplicial spheres ∆,this quantity is known [30]to coincide with the signature or index of the associated toric variety X ∆.Conjecture 1.3(Charney-Davis,Conjecture D [11]).When ∆is a flag simplicial homology (d −1)-sphere and d is even,then(−1)d2h (−1)≥0.Proof.Since h (t )has degree d we have h d =0and by symmetry h 0=0.Thus h (t )has d zeroes which must then all be strictly negative since h i ≥0for 0≤i ≤d .Factor h (t )=h d di =1(t −r i )according to its(real)zeroes r i .Symmetry of h (t )implies that r is a zero if and only if 1r is less than −1.Thus for a zero r ,either r =−1is a zero,in which case h (−1)=0and we are done,or else exactly half of the factors in the product h (−1)=h d d i =1(−1−r i )are negative,implying that the product has sign (−1)d 2W (P,−1),for some cases of posets where the Neggers-StanleyConjecture is known,are explored in [36].In Section 3.2it is shown that the sphere ∆eq (P )is the boundary complex of a simplicial convex polytope.Therefore by McMullen’s g -Theorem characterizing the number of faces of such polytopes [40],the coefficients (h 0,h 1,...,h #P −r )are symmetric and unimodal.Convexity has further relevance.In [30]it was shown via the Hirze-bruch signature formula that the Charney-Davis Conjecture holds forCHARNEY-DAVIS AND NEGGERS-STANLEY CONJECTURES5 a simplicial polytope under a certain geometric hypothesis(local con-vexity)stronger than beingflag.We show in Section3.2that this hypothesis holds for∆eq(P)whenever P has width(i.e.size of the largest antichain)at most2,thereby providing more evidence for the Neggers-Stanley Conjecture.In Sections4and5we gather evidence for the thesis that both of these conjectures can be fruitfully viewed within the context of Koszul algebras.In particular,we point out ways in which Hilbert series of Koszul algebras interact well with the theory of Polya frequency series and polynomials with real zeroes.After this paper was circulated,C.Athanasiadis[1]has shown that the unimodular triangulation of the order polytope from Section3.1 is a member of a class of triangulations of polytopes that decompose into a join of a simplex and a polytopal sphere.Most notably he has exhibited such a triangulation for the Birkhoffpolytope.2.Review:P-Partitions and Order PolytopesIn this section we review some of the theory of P-partitions,distribu-tive lattices and order polytopes;see[25,27,26,39,41]for proofs and more details.Also see[18,§1.2]for definitions and basic facts about polyhedral cones and fans.Given a naturally labelled poset P on[n]ordered by≤P,the vector space of functions f=(f(1),...,f(n)):P→R will be identified with R n.One says that f is a P-partition if f(i)≥0for all i and f(i)≥f(j) for all i<P j.Denote by A(P)the cone of all P-partitions in R n.The convex polytopeO(P)=A(P)∩[0,1]nis called the order polytope of P.An order ideal I in P is a subset of P such that i∈I and j<P i implies j∈I.It is known that O(P)is the convex hull of the characteristic vectorsχI∈{0,1}n as I runs through all order ideals I in P.A useful alternative way to view O(P)is provided by the fact that it is isometric to the hyperplane slice at x0=1of the cone A(P0)⊂R n+1,where P0is the naturally labelled poset on[0,n]:={0,1,...,n} obtained from P by adjoining a new minimum element0.We call the cone A(P0)the homogenization of the cone A(P).We recall a few basic definitions some of which were already men-tioned in the introduction.The set of permutations w=(w1,...,w n)∈S n which extend P to a linear order is called its Jordan-H¨o lder set L(P):= w=(w1,...,w n)∈S n:i<P j implies w−1(i)<w−1(j) .6VICTOR REINER AND VOLKMAR WELKERThe descent set and descent number of w are defined byDes(w):={i∈[n−1]:w i>w i+1}des(w):=#Des(w).Define a cone for each w∈S nA(w):={f∈R n:f(w i)≥f(w i+1)for i∈[n−1],f(w i)>f(w i+1)if i∈Des(w)}It is not hard to see that the closure of A(w)(defined by removing the strict inequalities above),is a unimodular(simplicial)cone,that is its extreme rays are spanned by a set of vectors forming a lattice basis for Z n.Similarly,the closure of A(w)∩[0,1]n is a unimodular simplex. Now we are in position to formulate the basic fact from the theory of P-partitions which will be crucial for subsequent arguments. Proposition2.1.(i)The cone of P-partitions decomposes into a disjoint union asfollows:A(P)=⊔w∈L(P)A(w)The closures of the cones A(w)for w∈L(P)give a unimodulartriangulation of A(P).(ii)The unimodular triangulation of A(P)described in(i)restricts to a unimodular triangulation of the order polytopeO(P)=⊔w∈L(P)A(w)∩[0,1]n.We call the triangulations of A(P)(into simplicial cones)and O(P) (into simplices)from Proposition2.1their canonical triangulations. Note that via homogenization the canonical triangulation of O(P)is easily seen to be the restriction of the canonical triangulation of the homogenized cone A(P0)to the hyperplane x0=1.This makes sense since there is an obvious bijection between the linear extensions L(P0) and L(P).The combinatorics of these triangulations is closely related to the distributive lattice J(P)of all order ideals I in P ordered by inclusion. The order complex∆J(P)is the abstract simplicial complex having a vertex for each ideal I in P and a simplex for each chain I1⊂...⊂I t of nested ideals.Given a set of vectors V⊂R n,define their positive span to be the(relatively open)conepos(V):= v∈V c v·v:c v∈R,c v>0 .CHARNEY-DAVIS AND NEGGERS-STANLEY CONJECTURES7Proposition2.2.(i)Every non-zero P-partition f∈A P can be uniquely expressedin the formf=t i=1c iχI iwhere the c i are positive reals,and I1⊂···⊂I t is a chain ofideals in P.In other words,A(P)= ideals I1⊂···⊂I t⊂P pos {χI t}t i=1 .(ii)The canonical triangulation of the order polytope O(P)is iso-morphic(as an abstract simplicial complex)to∆J(P),via anisomorphism sending an ideal I to its characteristic vectorχI.(iii)The lexicographic order of permutations in L(P)gives rise to a shelling order on∆J(P).(iv)In this shelling,for each w in L(P),the minimal face of its cor-responding simplex in∆J(P)which is not contained in a lexico-graphically earlier simplex is spanned by the ideals{w1,w2,...,w i}where i∈Des(w).Using basic facts about shellings(see[4]),part(iv)of the preceding proposition implies that one can re-interpret the polynomial W(P,t): (2.1)W(P,t):= w∈L(P)t des(w)=h(∆J(P),t)This connection with J(P)also allows one to re-interpret these re-sults in terms of Ehrhart polynomials.Recall that for a convex poly-tope Q in R n having vertices in Z n,the number of lattice points con-tained in an integer dilation dQ grows as a polynomial in the dilation factor d∈N.This polynomial in d is called the Ehrhart polynomial: Ehrhart(O(Q),d):=# d O(P)∩N n .Whenever Q has a unimodular triangulation abstractly isomorphic toa simplicial complex∆,there is the following relationship:(2.2) d≥0Ehrhart(O(Q),d)t d=h(∆,t)8VICTOR REINER AND VOLKMAR WELKERthe equatorial triangulation.This triangulation has several pleasant properties,proven in this and the next subsection,which may be sum-marized as follows:⊲It is a unimodular triangulation.(See Proposition3.6)⊲It is isomorphic,as an abstract simplicial complex,to the joinof an r-simplex with a simplicial(#P−r−1)-sphere,which wewill denote∆eq(P),and call the equatorial sphere.(See Corollary3.8)⊲h(∆eq(P),t)=h(∆J(P),t)=W(P,t).(See Corollary3.8)⊲The equatorial sphere∆eq(P)is polytopal,and hence shellableand a PL-sphere.(See Theorem3.14)⊲When P has width at most2,the equatorial sphere∆eq(P)is realized by a locally convex simplicial fan.Hence is aflagsubcomplex of∆J(P),and aflag sphere for which the Charney-Davis Conjecture holds.(See Theorem3.23)Example3.1.Let P be the graded naturally labelled poset on[4] with r=2ranks shown in Figure1(a).Let J(P)be its associated (distributive)lattice of order ideals(see Figure1(b)).The4-dimensional order polytope O(P),and its canonical triangula-tion by∆J(P),may be“visualized”as follows.Start with the convex pentagonπwhich is the convex hull of{χ1,χ2,χ12,χ13,χ123,χ124},and triangulateπas shown in Figure1(c).The canonical triangulation is obtained by taking the simplicial join of this triangulation ofπwith the edge{χ∅,χ1234}.The equatorial triangulation(see Proposition3.6)is obtained start-ing from the alternate triangulation ofπdepicted in Figure1(d)and taking the simplicial join with the edge{χ∅,χ1234}.Equivalently,it is obtained from the equatorial1-sphere∆eq(P)depicted in Figure1(e) and taking the simplicial join with the triangle{χ∅,χ12,χ1234}.Fix a naturally labelled poset P on[n],and assume that it is graded, with r rank sets P1,...,P r.The following are the key definitions.Definition3.2.A P-partition f will be called rank-constant if it is constant along ranks,i.e.f(p)=f(q)whenever p,q∈P j for some j.A P-partition f will be called equatorial if min p∈P f(p)=0and for every j∈[2,r]there exists a covering relation between ranks j−1,jCHARNEY-DAVIS AND NEGGERS-STANLEY CONJECTURES9Figure 1.(a)A graded poset P .(b)The distributivelattice of order ideals J (P ).(c)Part of the canonicaltriangulation ∆J (P )of its order polytope O (P ).(d)The analogous part of the equatorial triangulation.(e)The equatorial 1-sphere ∆eq (P ).in P along which f is constant,i.e.there exist p j −1<P p j withp j −1∈P j −1,p j ∈P j and f (p j −1)=f (p j ).An order ideal I in P will be called rank-constant (resp.equatorial )if its characteristic vector χI is rank-constant (resp.equatorial).More generally,a collection of ideals {I 1,...,I t }forming a chain I 1⊂...⊂I t will be called rank-constant (resp.equatorial )if the sum χI 1+...+χI t (or equivalently,any vector in the cone pos({χI j }t j =1)is rank-constant (resp.equatorial).Note that the only rank-constant ideals are the ones in the chain∅=I rc 0⊂I rc 1⊂···⊂I rc r =P10VICTOR REINER AND VOLKMAR WELKERwhere I rc j:=⊔i≤j P i.Also note that the only P-partition which is both rank-constant and equatorial is the zero P-partition f(p)=0.Thus the only rank-constant and equatorial order ideal is I rc0=∅. Proposition3.3.Every non-zero P-partition f can be uniquely ex-pressed asf=f rc+f eq,where f rc,f eq are rank-constant and equatorial P-partitions,respec-tively.Proof.To show existence,for j∈[r−1]define non-negative constantsc j:=min{f(p j−1)−f(p j):p j−1∈P j−1,p j∈P j,p j−1<P p j}c r:=min{f(p r):p r∈P r},and setf rc:=r j=1c jχI rc jf eq:=f−f rc.Obviously f rc is a rank-constant P-partition.It is a straightforward verification,left to the reader,that f eq is a P-partition,and that it is equatorial by construction.For uniqueness,assume f=g rc+g eq is an additive decomposi-tion of f into a rank-constant and an equatorial P-partition.It is again straightforward to show that the equatoriality of g eq and rank-constancy of g rc forces g rc= r j=1c jχI rc j,where c j is defined as above in terms of f.We wish to deduce our equatorial triangulation of A(P)from Propo-sition3.3,and for this we need to understand both rank-constant and equatorial chains of ideals better.Equatoriality and rank-constancy of a chain of ideals I1⊂...⊂I t are intimately related with properties of its jumpsJ i:=I i−I i−1for i=1,...,t+1(where by convention I0:=∅,I t+1=P).It is easy to see that the rank-constant P-partitions form an r-dimensional simplicial subcone within the n-dimensional cone A(P), and that this subcone is the non-negative span of the vectors{χI rcj}r j=1. Proposition3.4.The rank-constant subcone of A(P)is interior,that is,it does not lie in the boundary subcomplex of the cone A(P). Proof.In a triangulation of a polyhedral cone,a subcone lies on the boundary if and only if it is contained in a codimension one subcone that lies on the boundary.For codimension one subcones,lying in theCHARNEY-DAVIS AND NEGGERS-STANLEY CONJECTURES11 boundary is equivalent to being contained in a unique top dimensional subcone.Specializing to the case of the canonical triangulation of the cone A(P)from Proposition2.1,one sees that this means a chain of ideals I1⊂···⊂I t corresponds to a subcone on the boundary if and only if one of at least one of its jumps J i contains a pair of elements which are comparable in P.But for I rc1⊂···⊂I rc r,since the jumps J i=I rc i−I rc i−1=P i are antichains,this property fails to hold. Proposition3.5.A chain of non-empty ideals I1⊂...⊂I t,is equa-torial if and only if its jumps J i have the following property:For every j∈[2,r],there exist p j−1<P p j with p j−1∈P j−1,p j∈P j and a value i∈[t+1],such that p j−1,p j∈J i.The chain I1⊂...⊂I t is maximal with respect to the equatorial property if and only if its jumps J i for i∈[t+1]satisfy the following two conditions:(i)The J i are all maximal(saturated)chains in P,possibly single-tons.(ii)The non-singleton J i can be re-ordered J i1,J i2,...,J isso thatmin Ji1has rank1,max Ji shas rank r,and max J ik,min J ik+1have the same rank in P for k∈[s−1].Consequently,t=n−r for any maximal equatorial chain of non-empty ideals.Proof.Since the jumps J i are the domains on which the associated P-partitionχI1+...+χItis constant,thefirst assertion is direct fromDefinition3.2.It is then easy to see that a chain of non-empty ideals having proper-ties(i),(ii)will be equatorial,and maximal with respect to refinement.Conversely,suppose one is given a maximal equatorial chain of non-empty ideals.If there exists an incomparable pair p,p′in one of its jumps J i,it is straightforward to check that one can refine the chainfurther while preserving the equatorial property,e.g.by adding in theideal I i−1∪{q∈J i:q≤p}.Thus each jump J i must be a maximalchain,proving(i).Furthermore,the pairs of adjacent ranks{j−1,j} spanned by two different jumps J i,J i′must be disjoint,else one could refine the chain equatorially by“breaking”J i between two such ranks{j−1,j}which they share.The jumps J i must then disjointly coverall possible adjacent rank pairs{j−1,j}r j=2,so they can be re-ordered as in(ii). Proposition3.6.The collection of all conespos {χI:I∈R∪E} ,12VICTOR REINER AND VOLKMAR WELKERwhere R(resp.E)is a chain of non-empty rank-constant(resp.equa-torial)ideals in P,gives a unimodular triangulation of the cone of P-partitions A(P).Proof.First we check that these polytopal cones indeed decompose A(P).Given f∈A,write f=f rc+f eq as in Proposition3.3.Then use these easy facts:⊲f rc lies in the cone of rank-constant P-partitions,which is thesimplicial cone positively spanned by the(non-empty)rank-constant ideals{I rc j}r j=1,⊲When f eq is expressed in the unique way as a positive combina-tion of characteristic vectors of a chain of ideals,as in Propo-sition2.2part(i),this chain of ideals must be equatorial sincef eq is.It remains to check that all such cones are unimodular.Thus it suffices to show that whenever R∪E is maximal under inclusion,then #R∪E=n and the Z-span of the set{χI:I∈R∪E}additively generates inside R n is the full integer lattice Z n.To see#R∪E= n,first note that when R∪E is maximal,one has R={I rc j}r j=1, and then#E=n−r follows from Proposition3.5.To show they additively generate Z n,we show by induction on the rank r of P that the subgroup they generate contains each standard basis vector e p for p∈P.The base case r=1has P an antichain,hence all ideals I P are equatorial,so the cones in question coincide with the cones in the canonical triangulation,which are unimodular by Proposition2.1.In the inductive step,note that this subgroup generated by{χI:I∈R∪E}has the alternate description as the subgroup generated bythe characteristic vectorsχPj of all of the ranks of P along with thecharacteristic vectorsχJi of all of the jumps between the equatorialideals in E.Proposition3.5shows that there will be exactly one element q of the top rank r in P which does not occur in a singleton jump J i.Namely,q=max J is after the re-labelling as in Proposition3.6.Hencefor every p∈P r−{q},one has e p in the subgroup,but then one alsohas e q in the subgroup,since the subgroup containsχPr .Now applyinduction to the graded poset P−P r of rank r−1,replacing the ideals in R∪E by their intersections with P−P r and removing multiple copies of the same ideal created by the intersection process. The triangulation of A(P)given in Proposition3.6induces a uni-modular triangulation of O(P),which we will call the equatorial trian-gulation of O(P).CHARNEY-DAVIS AND NEGGERS-STANLEY CONJECTURES13 Definition3.7.The equatorial complex∆eq(P)is defined to be the subcomplex of the order complex∆J(P)whose faces are indexed by the equatorial chains of non-empty ideals.For the formulation of the next corollary we need the concept of simplicial join.For two simplicial complexes∆1,∆2which are defined over disjoint vertex sets,the simplicial join∆1∗∆2is the simplicial complex{σ1∪σ2:σi∈∆i,i=1,2}.Note that we always assume that the empty face∅is a face of a simplicial complex.Corollary3.8.The equatorial triangulation of the order polytope O(P) is abstractly isomorphic to the simplicial joinσr∗∆eq(P),whereσr is the interior r-simplex spanned by the chain of rank-constant ideals {I rc j}r j=0.As a consequence of its unimodularity,one hash(∆eq(P),t)=h(∆J(P),t)=W(P,t).Proof.Thefirst assertion follows directly from Proposition3.6,noting thatσr is interior due to Proposition3.4.For the second,note that bothσr∗∆eq(P)and∆J(P)index unimodular triangulations of the order polytope,so(2.2)impliesh(σr∗∆eq(P),t)=h(∆J(P),t).On the other hand,the defining equation(1.1)of the h-polynomial shows thatf(∆1∗∆2,t)=f(∆1,t)∗f(∆2,t)h(∆1∗∆2,t)=h(∆1,t)∗h(∆2,t)h(σr,t)=1,and hence h(σr∗∆,t)=h(∆,t). Remark3.9.Corollary3.8has the following consequence:for a graded poset P, the set of linear extensions L(P)is equinumerous with the set L eq(P) of all maximal equatorial chains of ideals in P,as both coincide with [W(P,t)]t=1.This begs for a bijectionφ:L(P)→L eq(P).The authors thank Dennis White[53]for supplying one which is elegant,using the idea of jeu-de-taquin on linear extensions of P,thought of as P-shaped tableaux that use each entry1,2,...,n exactly once.Given such a linear extension w,replace the highest label n(at top rank r)by a jeu-de-taquin hole,and slide it past other entries down to rank1,du-plicating the last entry that it slid past in the hole’s resting position at rank1.Then repeat this with the entry n−1,sliding it down to rank2,and similarly with the entries n−2,n−3,...,n−r+1.The14VICTOR REINER AND VOLKMAR WELKERresult is a P-shaped tableaux that can be interpreted as an equato-rial P-partition,compatible with a unique maximal equatorial chain of idealsφ(w).It is not hard to check that this map w→φ(w)is a bijection.3.2.Geometric and Convexity Properties of∆eq(P).In this sec-tion,we use convexity and the concrete geometric realization of∆eq(P) to learn more about it.Definition3.10.The rank-constant subspace V rc⊂R n is the R-linear}r j=1.span of the set{χI rcjLet Q be a convex polytope,and V a linear subspace,both inside R n.Then there is a well defined quotient polytopeQ/V:={q+V:q∈Q}⊂R n/V.Ifπ:R n→R n−dim V is any linear surjection with kernel V(such as an orthogonal projection onto V⊥),then the polytope Q/V can be identified with the imageπ(Q).Also note that if V is a rational subspace of R n with respect to the integer lattice Z n⊂R n,the quotient lattice Z n/(V∩Z n)is well-defined,and a full rank sublattice in R n/V. Proposition3.11.The collection of quotient conesC E=pos {χI:I∈E} +V rc ,as E runs through all equatorial chains of non-empty ideals in P,forms a complete simplicial fan in R n/V rc.(i)This simplicial fan is unimodular with respect to the quotientlattice Z n/(V rc∩Z n).(ii)The simplices(C E∩O(P))+V rc form a unimodular triangula-tion of the quotient polytope O eq(P):=O(P)/V rc.(iii)This triangulation of O(P)/V rc is isomorphic,as an abstract simplicial complex,to the cone0∗∆eq(P)with base∆eq(P)andapex at the interior point0=V rc.Consequently,∆eq(P)triangulates the(n−r−1)-dimensional bound-ary sphere∂O eq(P).Proof.Apply the following general statement,Proposition3.12,about polytopes(and the analogous statement about fans)withQ=O(P),∆=the equatorial triangulation,∆′=∆eq(P),V=V rc.CHARNEY-DAVIS AND NEGGERS-STANLEY CONJECTURES15Proposition3.12.Let Q be an n-dimensional convex polytope in R n. Assume Q has a triangulation abstractly isomorphic to a simplicial complex∆of the form∆∼=σr∗∆′,whereσr is an r-simplex not lying on the boundary of Q.Let V be the r-dimensional linear subspace parallel to the affine span of the vertices ofσr.Then the quotient(n−r)-dimensional polytope Q/V⊂R n/V in-herits a triangulation abstractly isomorphic toσ0∗∆′,whereσ0is an interior point of Q/V⊂R n/V.Furthermore,when V is rational with respect to Z n⊂R n and if the triangulation of Q is unimodular with respect to Z n,then the triangu-lation of Q/V rc is unimodular with respect to Z n/(V rc∩Z n).The proof of Proposition3.12is straightforward.We leave it as an exercise.Proposition3.11,shows that∆eq(P)corresponds to a complete uni-modular fan.This fact suffices to infer both that it is spherical,andthat it corresponds to a smooth,complete toric variety X∆eq(P)(see[18,§2.1]).Our next goal will be to show that∆eq(P)corresponds to a polytopal fan,as this has multiple consequences;see Corollary3.15 below.We prove polytopality of∆eq(P)by choosing for each equatorial ideal I of P a point on its ray pos(χI+V rc)so that the convex hull of all such points is a simplicial polytope having∆eq(P)as its boundary complex.Here we employ the following strategy.We start with the (usually)non-simplicial polytope O eq(P)and pull each of its vertices in a certain order to produce a simplicial polytope with boundary complex ∆eq(P).Recall[31,§2.5]that if Q is a convex polytope,one pulls the vertex v in Q to produce a new polytope pull v(Q)by taking the convex hull after moving v slightly outward past the supporting hyperplanes of all facets that contain v,but past no other facet-supporting hyperplanes of Q.Assuming that Q contains the origin in its interior,this can clearly be achieved by replacing v with(1+ǫ)v whereǫ>0is sufficiently small.We will require the following proposition describing the1-skeleton resulting from pulling all the vertices of a polytope: Proposition3.13.Let Q be the polytope resulting from pulling all of the vertices of a polytope Q in some order v1,v2,...,and let v i denote the corresponding vertices in Q.。
罗兰(Roland)FR-8x V-Accordion商品介绍说明书
The Ultimate Fusion of Technology and TraditionWith the incredible new FR-8x, Roland has perfected the synergy between traditional accordion playability and modern digital power. The latest flagship piano-type V-Accordion is jam-packed with features and enhancements developed with input from the world’s top players, bringing a previously unattained level of expression and versatility to every accordionist. Innovative Dynamic Bellows Behavior technology delivers the true bellows response of an acoustic accordion, while the expanded sound set, four powerful multi-effects, anonboard looper, and much more offer atreasure chest of tools for dynamic musical exploration. Seamlessly fusing top-level technology with familiar acoustic tradition, the FR-8x V-Accordion ushers in a new era of creative freedom for players everywhere.Flagship piano-type V-Accordion, filled with many enhancements requested by pro accordionistsNewly developed Dynamic Bellows Behavior technology emulates the true bellows response of an acoustic accordion in every registerSimple and convenient onboard battery charging with an AC adapterA large selection of accordion sounds from around the world, plus 180 orchestra and percussion sounds and world-class Virtual Tone Wheel organsFour powerful multi-effects engines (MFX), with dedicated MFX for Accordion, Orchestra 1, Orchestra 2, and Orchestra Chord sections.All-new user interface, featuring a large, easy-to-read color display, intuitive panel layout, and three programmable chin switches for hands-free control of a variety of functions1400 user program memories allow players to save custom setups for every performing situation Onboard looper for creating instant backing accompanimentRecording and audio playback via convenient USB memory; USB host port for connecting to computers Available in red and black finishes■■■■■■■■■■mp3True Acoustic Response with Dynamic Bellows BehaviorRedesigned Interface with Color Display and Intuitive Panel LayoutAll-in-One Operation and Onboard Battery ChargingNewly developed for the FR-8x, Dynamic Bellows Behavior technology represents a real breakthrough for digitalaccordionists. In an acoustic accordion, sounds are produced by reeds that vibrate with airflow generated by the movement of the bellows; the resistance of the bellows constantly varies, depending on how many reeds are selected and how many notes are played at once. In the FR-8x, Dynamic BellowsBehavior automatically adjusts the air transfer in the bellows in real time based on the selected register and the number of notes played, accurately replicating the familiar andcomfortable bellows feel of an acoustic accordion. Dynamic Bellows Behavior can be easily disabled for players that prefer the bellows feel of previous V-Accordions.The FR-8x features a completely redesigned user interface that’s more powerful and easier to use than ever before. A large, recessed color display makes it simple to see and edit various parameters, while the revamped panel layout provides fast, intuitive operation via many dedicated buttons and knobs. 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In addition, all device connections are now located right on the instrument, including MIDI, USB, and audio jacks for connecting to an external amplification or recordingsystem.Expanded Collection of World-Class SoundsZones, Layers, and DrumsPowerful Multi-Effects and Onboard LooperIn addition to a full selection of authentic accordion sounds from around the world, the FR-8x is equipped with over 180 orchestra and percussion sounds, giving you the power to expand your music into unexplored territory. Included are traditional instruments such as strings and brass, plus electric and acoustic guitars, choir, church organ, harp, ethnic sounds, synthesizers, and a wide range of drum kits. With the Virtual Tone Wheel sound engine, you can play amazing organ sounds using Treble (upper), Chord (lower) and Bass (pedal) sections, with harmonic bar controls to personalize your organ sounds for any musical style. Four internal memory areas (8 MB each) are provided for loading new sounds from the Roland sound library.With the FR-8x, more layering and zone setup options are possible in the right-hand keyboard modes than ever before. Whole, Zone, High, and Low modes are provided, giving you the ability to play up to four different tones at once. Left-hand keyboard modes now include layering options as well. The programmable Drum function takes accordion performance to a fun new dimension, letting you play percussion sounds manually with the Bass & Chord buttons.Explore all-new sonic textures with the FR-8x’s fourindependent multi-effects engines (MFX), which provide dedicated processing for the Accordion, Orchestra 1,Orchestra 2, and Orchestra Chord sections. Each engine has 84 different effects types, offering a wide range of enhancement from subtle to dramatic. With the onboard looper, you can instantly record and overdub accordion performances using the FR-8x’s enormous selection of sounds, creating impressive,on-the-spot backing accompaniment for improvisation.USB Song Playback, Recording, and MoreThe handy MP3/WAV song player lets you play along with pre-recorded musical tracks for practice and live backing via optional USB memory. Just plug your USB stick into the convenient front-panel plug, then select and play songs with dedicated, easy-to-reach controls. And with the touch of a button, your accordion performances can be recorded directly to USB memory as well, perfect for archiving, evaluation, and education. Via the USB host port on the side panel, you can connect the FR-8x to your computer for data storage, customization ofV-Accordion sound sets, and easy-to-install software updates.[Keyboard, Bass & Bellows]- Right Hand41 keys piano type with velocity sensitive and aftertouch- Left Hand120 bass buttons velocity sensitive. Standard, Free Bass mode, Orch. Bass, Orch. Chord, Orch. Free Bass.- Bass & Chord Mode2 Bs Rows,3 Bs Rows A-7th, 3 Bs Rows A-5dim, 3 Bs Rows B-7th, 3 Bs Rows B-5dim, 3 Bs Rows Bx-7th , 3 Bs Rows Belgium- Free Bass ModeMinor 3rd, Bajan, Fifth, North Europe, Finnish- BellowsAdvanced “Dynamic Bellows Behavior” technology to manage the behavior of bellows.- Bellows ResistanceOn, Off, -63 to 0 to +64- Bellows CurveFixed Low, Fixed Med, Fixed High, X-Light, Light, Standard, Heavy, X-Heavy[Sound Source]- Max Polyphony128 voices- Tones (Accordion Set)100 Accordion Sets, each one including: 14 Treble Registers, 7 Bass/Chord registers, 7 Free Bass registers, 7 Orchestra Free Bass registers, 7 Orchestra Bass registers, 7 Orchestra Chord registers, 180 Orchestral sounds (28 real time + others selectable by MENU), 18 Drum Sets- Reed Footages7 Treble, 5 Bass, 3 Chord, 2 Free Bass- Additional SoundsUploadable from USB memory and saved on internal memory[Orchestral Sounds]180: 28 real time (14x2) the others selectable by MENU[Organ Sounds (Virtual Tone Wheel)]32 presets for Treble, Chord and Free Bass sections, 16 presets x Bass section.Up to 28 Harmonic Bar combinations customizable, can be controlled and shaped by bellows.[Orchestral Bass Sounds]180: 7 real time, the others selectable by MENU[Orchestral Chord Sounds]180: 7 real time, the others selectable by MENU [Orchestral Free Bass Sounds]180: 7 real time, the others selectable by MENU[Drum Sets]18[User Programs]1400: 100 User Program Bank x 14 registers[APBM (Advanced Physical Behavior Modeling)]- NoisesStopping-reed growl, Closing valve noise, Left button noise- Individual Reed SimulationHysteresis threshold, Expression curve, Pressure variant filter, Pressure variant pitch deviation- Switching Reed Sound WaveBy bellows accelerationBy note repetition speed- Bellows Opening/Closing Sound ChangeBy bellows opening/closing detection- Bellows BehaviorDynamic Bellows Behavior technology for a perfect simulation of the bellows behavior in an acoustic accordion[Musette Tuning]- Micro-Tuning Presets16 Types: Off, Dry, Classic, F-Folk, American L/H, North Europe, German L/H, D-Folk L/H, Alpine, Italian L/H, French, Scottish- Fine Tuning Reed Footages 8- / 8+-100 to 0 to +100[Effects]- Reverb/Chorus/Delay8 types, 8 types, 10 types- MFX Multi EffectsMFX x 4 (84 types) for: Accordion, Orchestra 1, Orchestra 2, Orch Chord/Orch Free Bass- Rotary for Organ SoundSlow/Fast with Vibrato, Chorus, Overdrive and VK-Rotary- “Cassotto” SimulationYes[Panel Controls]- Knob Controls & RegistersVolume, Balance, Reverb Chorus, Delay, Effect (assignable knob), 14 x Accordion/Orchestra1/Orchestra2/OrganFR-8x Specifications- EncoderData Edit with Enter- Navigation SwitchesUp, Down, Menu/Write, Exit/Jump- Other SwitchesSet Up, Set Down, Orch 1 On/Off, Orch 2 On/Off, Organ On/Off, Accordion On/Off, Orch Bass On/Off, Orch Chord/Free Bass On/Off, Free Bass On/Off, Bass&Chord On/Off, Drums On/Off, Bass to Treble On/Off, User Program On/Off, Song List On/Off, Power On/Off, Charge On/Off, Loop/Wave/MP3 player: Loop, Reset/Stop, Play/ Pause, Audio Rec- Chin Switches3 programmable chin switches- Additional Switches6 user assignable function switches on last row of bass buttons[Operation Mode]- Accordion, Orchest1/Organ, Orchest2, DrumZone, High, Low- Octave-1, 0, +1 for Treble, -3, 0, +3 for Orchest1, Orchest2- Drum Shift-36 to 0 to +36- Orchestra Chord Guitar ModeGtr Table1, Gtr Table2, Gtr Table3- Sound EditOrchest1, Orchest2, Orch Bass, Orch Chord, Orch Free Bass- Bass to TrebleOn/Off- Part MuteAccordion, Orchest 1, Orchest 2, Organ, Bass&Chord, Free Bass, Orch Bass, Orch Chord, Orch Free Bass- Bass & Chord with Drum/Percussion Sounds Programmable drum/percussion sounds for Bass/Orch Bass 2 rows, Chord/Orchestra Chord 4 rows.- Audio Player and Audio RECMP3/Wave player from USB memory and REC on USB- Audio LoopREC (with Overdub function) and Play- Speakers OffOn/Off adjustable via Menu parameter- Editing and WriteFull parameters for each section - New Graphic User Interface [MIDI Functions]- Ext. Seq. Playback (MIDI IN) or USB Computer Accordion, Bass&Chord, Orchest1, Orchest2, Organ, Orch Bass, Orch Chord, Orch Free Bass, ALL (Local Off function)- Start/Stop MIDI TXSend Start/Stop by pushing Alpha dial[Others]- Display ColourLCD 2,4” 320 x 240 pixel- Rated Power Output2 x 25W RMS- Speakers2 x 9 cm neodymium speakers2 tweeters- Wave Expansion4 internal areas (8Mb each) to load new sounds- Power SupplySupplied AC adaptor PSB-14U, rechargeable Ni-MH battery pack 24V-4500mAhExpected battery life under continuous use: 8-hours speaker ON mode, 11-hours speaker OFF mode- Onboard ConnectorsOUTPUT jacks L/Mono (Treble), R/Mono (Bass): 1/4”phone type, PHONES jack: 1/4” phone type, MIDI OUT connector, MIDI IN connector, USB MEMORY connector type A, USB COMPUTER connector type B, DC IN connector (use Roland PSB-14U AC adaptor only)- AccessoriesPSB-14U AC Adaptor, Power cord (for connectingthe AC adaptor), rechargeable Ni-MH battery pack24V-4500mAh, Owner's Manual, Reference caps for the bass buttons, Straps, Accordion Cloth, accordion soft bag- Options (sold separately)USB flash memory (M-UF-series), Headphones RH-200, RH-300, rechargeable Ni-MH battery pack 24V-4500mAh, external pedal footswitch- Colour VariationBlack, Red[Size and Weight]- Size415 (H) x 543 (W) x 280 (D) mm16-3/8 (H) x 21-7/16 (W) x 11-1/16 (D) inches- Weight12.1 Kg, 26 lbs 11 oz without strapsAll specifications and appearances are subject to change.FR-8x Specifications。
Module_1_PDA_Overview_052209_-_Chinese
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PDA programs and meetings contribute to global education, networking and harmonization PDA的程序和会议有助于促进全球教学、联系和一致性
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The interstellar medium in the edge-on galaxy NGC 5907
Astron.Astrophys.325,124–134(1997)ASTRONOMYANDASTROPHYSICSThe interstellar medium in the edge-on galaxy NGC5907Cold dust and molecular line emissionM.Dumke1,J.Braine2,3,M.Krause1,R.Zylka1,R.Wielebinski1,and M.Gu´e lin31Max-Planck-Institut f¨u r Radioastronomie,Auf dem H¨u gel69,D-53121Bonn,Germany2Observatoire de Bordeaux,URA352,CNRS/INSU,B.P.89,F-33270Floirac,France3Institut de Radioastronomie Millim´e trique,300rue de la Piscine,F-38406St.Martin d’H`e res,FranceReceived17February1997/Accepted18March1997Abstract.In this paper we present new observations of the interstellar medium in the non-interacting edge-on galaxyNGC5907.We have observed the J=2−1and J=1−0lines of the12CO molecule and radio continuum emission atλ1.2mm.The distribution of the molecular gas(as traced by CO)shows a maximum in the central region and a ring or spiral arm atr∼7kpc.Further analysis of the major axis distribution reveals evidence for an inner ring-like structure at r∼3.5kpc.Thekinematics can be described by rigid rotation in the inner part,a turnover at∼3kpc,and differential rotation with a velocityof230km/s in the outer disk.The observed continuum emission is mainly due to thermalradiation of cold dust with an average temperature of T d=18K,with a small gradient from20K to16K from the centre to theouter disk.This cold dust component is necessary to explain ourresults.The dust emission closely follows the molecular gas in thecentral region,but is also detected at large radii where no COcan be seen.In these regions the dust absorption cross sectionper H atom atλ1.2mm is estimated to beσHIλ∼4.510−27cm2, a value similar to that in the outer parts of other galaxies.From theλ1.2mm emission we estimated a molecularmass of NGC5907of0.9109M ,about50%smaller thanfrom the CO emission.By combining the CO and contin-uum data we found that the CO-H2-conversion ratio increaseswith galactocentric radius,from∼0.71020at the centre to ∼1.61020cm−2/K km s−1at r=7.5kpc.A comparison of NGC5907and other edge-on galaxies con-cerning gas distribution,central kinematics and dust propertiesis presented.Key words:galaxies:individual:NGC5907–galaxies:ISM–galaxies:kinematics and dynamics–infrared:galaxies–radio continuum:galaxies–radio lines:galaxiesSend offprint requests to:M.D.(mdumke@mpifr-bonn.mpg.de)1.IntroductionThe evolution of spiral galaxies and their properties are deter-mined by many processes.One of the most important pointsis the occurrence and time-scale of star formation,which de-pends mainly on the amount,composition,and distribution ofthe available raw material.This raw material consists of neutralgas in either atomic or molecular form.The amount of atomic hydrogen can easily be derived frommeasurements of the21cm line of HI.The mass of molecu-lar hydrogen,on the other hand,is usually determined indi-rectly by observing the lowest rotational transition of the COmolecule.The measured line intensities are converted into H2column densities using a conversion factor X=N H2/I CO(1−0). The estimated molecular mass,however,is quite uncertain be-cause X is still a matter of debate(e.g.Maloney&Black1988;Combes1991;Arimoto et al.1996).Observations of thermal dust emission at mm-wavelengthsprovide an alternative way to estimate the total mass of the in-terstellar matter of a spiral galaxy.Although this emission isdifficult to observe due to its weakness,it has several advan-tages.Firstly,at millimeter wavelengths the dust is opticallythin.Secondly,the emission scales roughly with thefirst powerof the temperature.Thirdly,at this wavelength the dust absorp-tion cross sections do not depend very much on physical dustproperties like grain size,shape,composition,and surface prop-erties(Hildebrand1983;Draine&Lee1984).And,finally,in-terstellar dust is about2orders of magnitude more abundantthan the most abundant CO molecule in normal spiral galaxies.In the last few years,the advent of multi-channel bolometerarrays has made it possible to obtain high quality maps(i.e.highangular resolution and high sensitivity)of the cold dust emissionof nearby spiral galaxies.In order to study the relation of thedust to the atomic and molecular hydrogen in a normal late-type spiral,we decided to observe the non-interacting edge-ongalaxy NGC5907.This galaxy shows a relatively low level of star formationfrom the weak infrared emission measured by IRAS(Young etM.Dumke et al.:The interstellar medium in the edge-on galaxy NGC5907125al.1989).Therefore it is–together with NGC4565observedby Neininger et al.(1996)–some kind of counterpart to themore active galaxies already observed in the radio continuumat mm-wavelengths:NGC891(Gu´e lin et al.1993),NGC3079(Braine et al.1997),NGC3627(Sievers et al.1994),NGC4631(Braine et al.1995),and M51(Gu´e lin et al.1995).NGC5907was observed in the HI-line twenty years ago andwas thefirst non-interacting galaxy where a galactic warp couldbe detected(Gu´e lin et al.1974;Sancisi1976).Former CO mea-surements(Sofue1994;Garc´ıa-Burillo&Gu´e lin1995)haveshown that this galaxy is relatively weak in CO.Although itsnearly edge-on orientation of i∼86◦.5does not allow us to ob-serve the emission of individual star forming regions or spiralarms in the disk,this inclination increases the column densityalong the line of sight to a significant and easier measurablevalue.Therefore NGC5907is a good candidate to study the ra-dial distribution of the dust and its correlation with the molecularand atomic hydrogen distributions.This will be done especiallyin comparison with the other non-interacting edge-on galaxiesmentioned above,namely NGC891and NGC4565.The latterone shows an even lower star formation activity than NGC5907and is also CO-weak,whereas NGC891contains a considerableamount of molecular gas and shows a relatively high level ofstar formation.These two galaxies are classified as Sb and Sbc,respectively,in contrast to the Sc-galaxy NGC5907.Furthermore edge-on galaxies are suitable to investigate thethickness of the gas and dust layer.Since NGC5907is lackingstrong star formation,one does not expect to detect a thick diskor halo in this galaxy because star formation and the existenceand structure of a gaseous halo seem to be directly connected(e.g.Dahlem et al.1995).In this paper we present our molecular line and bolometerobservations of NGC5907.The following section describes theobservations and the data reduction.Sect.3presents the resultswe obtained from the CO observations.In Sect.4we discussthe thermal dust emission.We estimate dust temperatures andabsorption cross sections,and compare the distribution of thecold dust with that of the atomic and molecular gas.From this weget some hints on how the CO-H2-conversion factor may vary ingalactic disks.In Sect.5the results for NGC5907are comparedwith those obtained for other edge-on galaxies,and thefinalsection gives a summary of our results and some concludingremarks.Table1lists some basic parameters of NGC5907which willbe used throughout this paper.2.Observations and data reductionThe observations presented here were all made with the30mtelescope of the Institut de Radio Astronomie Millim´e trique(IRAM),located on Pico Veleta(Spain).2.1.Molecular line observationsThe observations of the12CO(1−0)and the12CO(2−1)lineswere done in May1995and July1996.We used one3mm(two Table1.Some basic parameters of NGC5907Type Sc(de Vaucouleurs et al.1991)λ1.2mm centre:(this work)R.A.[1950]15h14m35s.7Dec.[1950]56◦30 37 .0Dynamical centre:(Garc´ıa-Burillo et al.1997)R.A.[1950]15h14m35s.5Dec.[1950]56◦30 43 .3v hel677km/s(Garc´ıa-Burillo et al.1997) Distance11Mpc(Sasaki1987)(1 corresponds to53pc)Pos.Angle155◦(Barnaby&Thronson1992)Incl.86.5◦(Garc´ıa-Burillo et al.1997)during the second observing period)and two1mm SIS receivers available at the30m telescope simultaneously.The receivers were tuned for image sideband rejections≥10dB(≥30dB at115GHz).The system temperatures were300-400K at 115GHz and500-700K at230GHz(in the T∗A scale).In the following we use main-beam line brightness temperatures T mb. These are converted from the antenna temperatures,corrected for atmospheric attenuation and rear spillover,T∗A,through T mb=T∗A/ηmb.The beam efficienciesηmb=B eff/F eff are0.73 and0.45for115and230GHz,respectively.The beamwidth was measured on Mars to be21 for the12CO(1−0)line and 11 for the12CO(2−1)line.The backends used consisted of two512×1MHz channelfilter banks,connected to one3mm and one1mm receiver,and an autocorrelator unit,connected to the other1mm receiver(and the other3mm receiver in July 1996).The observations were centered on the major axis of the galaxy.Adopting the central position from the bolometer ob-servations(given in Table1),we observed several points out toa projected radius of240 with12 spacings near the centre and24 spacings further out.Additionally we observed a few points above and below the major axis at distances of12 and24 from the plane.The observations were made by wobbling the subre-flector at a rate of0.5Hz between the source and a reference position located between±2 and±4 in azimuth(depending on the observing position and the orientation of the source).Some scans at larger radii were observed in the position-switching mode with on-and off-position located symmetrically around the center.Cold load calibrations were made every4-8minutes.During the CO observations we checked the pointing ac-curacy in two different ways.Firstly,we made pointing scans towards1641+399and1418+546every1-2hours.Sec-ondly,we measured(every∼2hours)small cuts perpendic-ular to the major axis at the center,consisting of three points at z=0 ,+12 ,and−12 ,and checked their symmetry,since the central point is expected to be strongest and the intensity of both off-axis points to be roughly equal.From these cuts and the pointing corrections made after each pointing scan we conclude that the mean pointing uncertainty is∼1 .5.The data reduction was done in a standard manner using the GILDAS software package.126M.Dumke et al.:The interstellar medium in the edge-on galaxy NGC59072.2.Bolometer observationsTheλ1.2mm observations were carried out in March1995withthe19-channel bolometer array developed at the Max-Planck-Institut f¨u r Radioastronomie,Bonn.The19channels are lo-cated in the centre and on the sides of two concentric regu-lar hexagons,with a spacing between two adjacent channels(beams)of20 .The central frequency and bandwidth of thebolometer are estimated to be245GHz and70GHz respec-tively(Gu´e lin et al.1995).For calibration purposes we haveobserved maps of Mars and Uranus during the bolometer obser-vations.These maps yielded a conversion factor from observedcounts to mJy/beam area of0.32mJy(beam area)−1count−1.The beamwidth at this frequency is∼10 .7.The continuum maps of NGC5907were observed in the Az-El coordinate system,with a scanning speed of4 /s in Azimuthwith data-acquisition every2 ,and a subscan separation of4in elevation.During the observations,the subreflector was wob-bled at2Hz in azimuth,with a beam throw of1 .The startingpoint of each subscan was shifted a few arcseconds in azimuthwith respect to the preceding one,which leads to a skewed shapeof each single coverage in the Az-El space,with two edges ofthe maps parallel to the major axis of the galaxy.This as wellas the use of different map sizes(between330 ×100 and 250 ×180 )was done in order to ensure that each subscan covers the galaxy and at least90 of blank sky on either side.We observed a total offifteen single maps of NGC5907,fivecentered on the optical centre(Barnaby&Thronson1992),theothers shifted164 along the major axis to the northwest andsoutheast,respectively.Since the optical centre and the centre oftheλ1.2mm emission(as found by our observations)differ bya few arcseconds,all offsets throughout this paper are relativeto the latter position which is given in Table1.During the bolometer observing session the pointing accu-racy was checked every1-2hours on1418+546.The pointingcorrections were always smaller than3 .The atmosphere wasrelatively stable and the sky opacity was∼0.2most of the time(always smaller than0.3).NGC5907was observed at relativelyhigh elevations(55◦-70◦)what reduces possible calibration er-rors,which are typically of the order15%.The data reduction was done with the MOPS software.Asecond order baseline wasfitted to each individual scan in az-imuth direction.Thefinal restoration was done applying the“mask-and-shift”restoring method,as outlined in the“PocketCookbook”(Zylka1996).3.Molecular gas in NGC59073.1.Observational results and kinematicsThe spectra along the major axis of the galaxy obtained duringthe molecular line observations are shown in Fig.1.The max-imum peak temperatures of∼0.33K and∼0.36K for theCO(1−0)and the(2−1)line respectively are reached near thecenter.CO is detected up to radii of more than200 (∼11kpc).A striking feature of many of the spectra(r≤80 )is thatthe observed lines contain at least two components,and thatthe Fig.1.Maps of the observed12CO(1−0)(left)and12CO(2−1)(right) major axis spectra of NGC5907,smoothed to a velocity resolution of 10.4km/s.The scale of the spectra is indicated by the small box at the bottom.Offsets are along the major axis,north is negativecentral spectrum shows a clear asymmetry.A natural explana-tion for the latter is that the location of the dynamical centre of the galaxy is not at x=0 (the centre of theλ1.2mm emission), but shifted by a few arcseconds to the northwest.This idea is also supported by the small asymmetry visible in the position-velocity diagrams(Fig.2).Garc´ıa-Burillo et al.(1997),who observed the central region of NGC5907using the Plateau de Bure interferometer,found the dynamical centre of the galaxy atα1950=15h14m35.s5,δ1950=56◦30 43. 3.This corresponds to(x,z)=(−6. 4,+1. 2)in our coordinates.They also found a small offset between the dynamical centre of the galaxy and theM.Dumke et al.:The interstellar medium in the edge-on galaxy NGC 5907127Fig. 2.Position-velocity diagram of the 12CO(1−0)(left)and the 12CO(2−1)(right)observations parallel to the major axis at z =0.Contour levels are -0.04(dashed),0.04,0.08,0.12,...,0.4K for both tran-sitions.The velocity resolution is 20km/s.The rms noise is variable along the major axis with a typical value of about 30mK for both transitions.The thick lines indicate the rotation curve as described in the text-200-100100200radius [arcsec]0204060d e p r o j e c t e d C O i n t e n s i t y [a .u .]-200-100100200x offset [arcsec]10203040I C O [K k m /s]Fig.3.a Observed (dashed line and filled black circles)and modelled (solid line)12CO(1−0)intensity distribution along the major axis of NGC 5907.The modelled distribution is obtained by a least-squares-fit and results from the line-of-sight-integrated radial distribution shown in b .b Adopted radial CO profile which leads to the major axis distribution as shown in aposition of the maximum CO intensity,which is in agreement with our results.The kinematics of NGC 5907can basically be described by rigid rotation up to a radius of ∼55 (which corresponds to ∼3kpc),followed by differential rotation with a rotational ve-locity of 230km /s.These values are relative to the systemic ve-locity of 677km /s and the dynamical centre given in Tab.1.The rotation curve follows from this work and the HI data (Caser-tano 1983)and is plotted as a thick line on the position-velocity diagrams (Fig.2).There are,however,a few deviations from this simple behaviour.A second line component is visible in the spectra near the central region (at |x |<30 ).Here the rigid (“normal”)rotation of the inner disk is accompanied by a high-velocity wing,with a much larger velocity gradient.This component is visible in the individual spectra as well as in the p -v -diagrams,and leads to a total line width of about 350km/s atthe assumed central position.It most probably results from non-circular motions due to a bar,as already suggested by Garc´ıa-Burillo &Gu´e lin (1995)and Garc´ıa-Burillo et al.(1997).3.2.Radial gas distributionThe observed major axis distribution of the CO intensity is the sum of the radial distribution and a projection effect (by which the emission at several radii is projected onto a certain position on the major axis).In order to deproject this distribution,we as-sumed a radial model function,consisting of a central Gaussian peak and two Gaussian rings,and fitted the resulting major axis distribution to the data.The existence of two ring-like struc-tures is suggested by two intensity maxima (at x ∼±60 and x ∼±120 )on either side of the centre in the p -v -diagrams.128M.Dumke et al.:The interstellar medium in the edge-on galaxy NGC5907Fig.4.Contour map of the continuum emission of NGC 5907at 245GHz,overlaid onto an optical image extracted from the Digitized Sky Survey.The beam size of 15 is indicated by the filled white circle in the lower right corner.The rms noise depends on the location in the map;on the galaxy it is about 1.5mJy/beam area,contour levels are 4,8,...,24mJy/beam area.The thin black lines indicate the λ1.2mm centre and the major axis of the galaxy as given in Table 1Additionally this distribution with two rings fits the data better than a distribution with just one ring (at r ∼120 ).The result can be seen in Fig.3.The best fit was obtained for ring radii of r 1=3.7kpc and r 2=7.0kpc and widths (FWHM)of Θpeak =4.4kpc,Θring1=1.4kpc,and Θring2=2.3kpc for the central peak and the inner and outer ring respectively.However,the outer “ring”may in fact be spiral arms seen more or less tangentially.4.Cold dust in NGC 59074.1.Observational resultsA contour map of the λ1.2mm continuum emission,overlaid onto an optical image extracted from the Digitized Sky Survey,is shown in Fig.4.This λ1.2mm-map is already smoothed to a beamsize of 15 to improve the signal-to-noise ratio.The emission is concentrated along a narrow ridge which follows closely the dusty optical disk,but is less extended,per-haps because of the sensitivity limit of our data.Although the emission is enhanced near the centre,there is no evidence for a nuclear point source.Several local maxima are visible along the major axis,but with some difference between the northern and the southern half.Whereas in the north there are three separatepeaks at projected radii of about 1 ,2 ,and 3.5,they seem to be somehow smeared out in the southern half,except the one atx ∼3 .5.In Fig.5we show the λ1.2mm continuum map,smoothed to a resolution of 21 HPBW,together with an HI total intensity map as received from Sancisi (m.),and the positions observed in the CO lines.NGC 5907is a really exemplary galaxy for the existence of galactic warps in neutral hydrogen (Sancisi 1976).It is,moreover,the first “normal”galaxy where a warp in the outer disk was observed.But in contrast to NGC 4565,another normal edge-on galaxy recently observed at λ1.2mm (Neininger et al.1996),no indication for a warp of the ther-mal dust emission can be seen (although the northernmost peak seems to be slightly shifted westwards with respect to the major axis).This may of course be due to the decreasing sensitivity at the outer edges of our dust map,which we reach at radii of ∼300 ,where the HI-warp is only marginally detected.4.2.ISM distributions along the major axisFig.6shows the distribution of the λ1.2mm continuum emis-sion along the major axis,together with the line intensities of the 12CO(1−0)and the HI emission.The spatial resolution of all three data sets is 21 ,as given by the 12CO(1−0)data.The continuum emission shows (more clearly in this plot than in the maps)the existence of two bright maxima at the end of the emission ridge (x ∼±200 )and of two less pronounced ones at x ∼±120 ,even if the southeastern one seems to be smeared out.Besides these similarities between the northern and the southern half the distribution is slightly asymmetric on smaller scales.The emission is detected up to radii of ∼250 in the south and even further,up to ∼280 ,in the northern half (with a significance of 2σ).Since there is λ1.2mm continuum emission beyond the edge of the CO disk,dust associated with the atomic component makes a significant contribution to the 1.2mm flux.The distribution of the CO line-intensities (and therefore the column densities of the molecular gas)shows also a maximum in the central region and decreases with increasing distance from the centre.Two further maxima are apparent at x ∼±120 .These features may be due to molecular rings and/or spiral arms in the inner part of the disk.The HI distribution shows a different behaviour.It has a minimum near the centre,increases at x ≤80 ,stays then roughly constant with several local peaks up to x ∼±200 ,and drops again further outwards.Hence this component is much more extended than the molecular gas in this galaxy.If we compare the dust emission with both gas phases,we find that it correlates with the molecular gas in the inner part ofM.Dumke et al.:The interstellar medium in the edge-on galaxy NGC5907129Fig.5.Contour maps of theλ1.2mm con-tinuum emission(left)and the HI line emis-sion(middle),as well as positions observed in the CO lines(right),all at the same scale and aligned in declination.The spatial reso-lution of the two maps is21 .Contour lev-els are3,7,12,18,25,33mJy/beam area for theλ1.2mm map and8,15,25,40,55, 701020atoms cm−2for the HI mapthe disk.At large radii,on the other hand,where CO is no longer detected,it seems to follow the HI emission.This result con-firms qualitatively that for NGC4565of Neininger et al.(1996). At smaller scales,wefind the two outer peaks in the dust emis-sion at x∼±200 corresponding to local maxima in the HI distribution,although there is a small displacement,especially on the southeastern side.From both CO peaks at x∼±120 only the northwestern one has a clear counterpart in the dust distribution,whereas in the southeastern half the dust emission shows just a small enhancement at this radius.4.3.Disk thicknessGarc´ıa-Burillo et al.(1997)estimated from their Plateau de Bure observations of the central region of NGC5907an inclina-tion of86.5◦and a thickness of the molecular disk of≤3 .In or-der to check if this is in agreement with our observations,wefit-ted the observed z-distribution(the averaged spectra are shown in Fig.7)with a Gaussian profiing the beamwidths given in Sect.2.1we determined a deconvolved thickness(FWHM) of the CO emission ridge of(13±5) ,somewhat thicker than in NGC4565(Neininger et al.1996).Additional off-axis ob-servations at x=60 have shown that this apparent thickness is nearly constant along the major axis.In order to estimate the extent of the atomic gas and the thermal dust emission perpen-dicular to the plane,we performed cuts along the minor axis of both maps.These lead to a mean beam deconvolved FWHM of the emission of(47±4) for the HI and(16±4) for the λ1.2mm emission.Since the galaxy is not perfectly seen edge-on,but under an inclination of i=86.5◦,a particular fraction of the off-axis emission is just projected from large radii to large z.We modelled this emission,using the radial CO profile obtained in Sect.3.2and a similar model,consisting of three rings,for the HI emission.The best agreement between model and data is found for a disk with a thickness(FWHM)of8 (which corresponds to∼400pc)for the CO and of28 (∼1.5kpc)for the HI.Both values seem to be unexpectedly large for a non-interacting spiral with only moderate star forming activity.We should note,however,that it is difficult to account for a warp in this simple modelling,and the results are very sen-sitive to the exact values of the inclination and the telescope beamwidth.Therefore,due to the large uncertainties,a thin molecular disk cannot be ruled out.4.4.Dust properties4.4.1.Non-dust contributions to the observedfluxUsing a ring integration method,we have determined the total flux density atλ1.2mm and found S1.2mm=605±55mJy.This value,however,cannot be attributed to thermal dust radiation alone.The broad band emission measured with the bolome-ter at245GHz rather consists of several components:thermal dust emission,free-free radiation,synchrotron radiation,and the CO(2−1)and some weaker lines.Since we are mainly in-terested in thefirst,we have to determine the contributions due to the other processes and to subtract them.The contribution of the12CO(2−1)line to the surface brightness measured with the bolometer can be calculated throughF line=2kν3c−3∆νbolΩbeam I CO(2−1)≈0.058I CO(2−1)(1) (with I CO(2−1)=lineT mb(12CO(2−1))dv in Kkms−1)for a bolometer bandwidth of70GHz and a beamwidth of11 for the continuum observations.With an assumed contribution of other isotopes and lines from other molecules of about10%of 12CO we estimate a totalflux density due to line contributions of S line=52±4mJy.The contribution of the continuum emission due to thermal and relativistic electrons is more difficult to determine since the130M.Dumke et al.:The interstellar medium in the edge-on galaxy NGC 5907300200100-100-200-300x offset [arcsec]010203040I C O [K k m /s ]SENW403020100I 1.2mm [mJy/b.a.]HI1.2 mmCO(1-0)Fig.6.The distribution of the 12CO(1−0)(thick dashed line,left scale)and the λ1.2mm continuum (thick solid line,right scale)along the major axis of NGC 5907.The HI distribution (thin solid line,arbi-trary units)is also shown.The spatial resolution in all three curves is 21radio continuum flux density at ν=1−10GHz originates partly in a double background source in the southern half of the galaxy (Hummel et al.1984;Dumke et al.1995).Furthermore the spectral behaviour of this background source is unknown,and the fraction of the galaxies’thermal emission is difficult to estimate.We used a total flux density of 47±5mJy at a frequency of 10.55GHz as derived by Dumke et al.(1995),a thermal fraction of 30%at this frequency and a nonthermal spectral index of −0.85which are typical for spiral galaxies (Niklas et al.1997)to calculate a value of S sync+ff =13±4mJy at 245GHz,which is about 2%of the total flux density.Besides these integrated values,we had to estimate the non-dust contributions along the major axis.The fraction of the CO lines,i.e.the line-to-continuum ratio,was calculated for each position from the CO(2−1)line following Eq.1and subtracted.Again we assumed that a fraction of 10%of the 12CO(2−1)-line stems from other lines in the bolometer band.For the free-free and synchrotron emission,we subtracted a fraction of 2%at each position,in accordance with the value estimated above.4.4.2.Dust temperaturesAfter subtracting the contributions of molecular lines and of synchrotron and free-free radiation,we determined a total flux density at 245GHz due to thermal dust emission ofS dust =540±60mJy .Including published IRAS flux densities (Young et al.1989)our observations allow to estimate color temperatures for the dust.We fitted a two-component modified Planck function to the data,using the points from 25µm to 1.2mm and under the assumption of a dust spectral index of 2(e.g.Chini et al.1986).The observed spectrum and the fitted curves (as well as their sum)are shown in Fig.8.The estimated temperatures for the two components to which we refer as cold and warm dust are 18K and 54K respectively.This result shows thatcoldFig.7.Averaged 12CO(1−0)and (2−1)spectra of the cuts through the centre.The portion of the spectra shown in each box ranges from v hel =300km /s to v hel =1000km /s and from T mb =−0.1K to T mb =0.4Kdust is necessary to explain the thermal continuum emission at λ1.2mm.The warmer dust alone which can be detected in the far-infrared by IRAS is not sufficient to account for the strong mm-emission and to explain our data.Although NGC 5907is a relatively inactive galaxy which does not show any signs of remarkable star forming activity (e.g.Dumke et al.1995),the dust emission is slightly enhanced at smaller galactocentric radii,and the dust may be somewhat warmer in this region.The FIR emission of NGC 5907was mapped by Wainscoat et al.(1987),using the IRAS CPC in-strument,at λλ50and 100µm with a resolution of 75 and 89 respectively.These maps were used to obtain spectra at different positions along the major axis of NGC 5907.We found that the temperature of the cold dust is somewhat higher in the central region (∼20K)than the value we got from the integrated flux densities,and drops to ∼16K at the outer disk.A similar de-crease is also found for other normal disk galaxies like NGC 891(Gu´e lin et al.1993),NGC 4565(Neininger et al.1996),or our Milky Way (Cox &Mezger 1989).。
Carl Zeiss SteREO Discovery.V8微观显微镜产品介绍说明书
M i c r o s c o p y f r o m C a r l Z e i s sSteREO Discovery.V8A New View of ThingsBrilliant Entry into the Class ofSophisticated StereomicroscopesSteREO Discovery.V8: Enhanced ViewingNew high-performance optics – this is the outstanding performance feature that Carl Zeiss has focusedon with the development of its latest entry levelmodel in the sophisticated stereomicroscope class.The SteR EO Discovery.V8 impresses with enhanced resolution, increased contrast and, most notably, a perceptibly improved stereoscopic impression. As aresult, it offers a image brilliance that is without equalin this class of instrument. For a visible increase in information in all biomedical and industrial applica-tions, the time has come for a new view of things.SteREO Discovery.V8at a glance:• Supreme ease of operation and ergonomicviewing posture• Zoom range of 8 : 1• Optimized optics design for a visible increasein image information• Manual focusing drive with adjustable clickstops• Manual and motorized stands with high stability• Generous specimen space with high workingdistance• Illumination and contrast methods based oncold light and LEDPCBLaterally grazing reflected light Objective: Plan S 1.0x Magnification: 16x*Mouth parts of the common houseflyOblique illumination in brightfieldtransmitted lightObjective: PlanApo S 1.0xMagnification: 80x*Wafer structureDarkfield reflected lightObjective: PlanApo S 1.5xMagnification: 120x*SteREO Discovery.V8stereoscopic impression of the microscopic image.Even on our SteREO Discovery.V8 entry level model.Another area we focused on during practical realiza-tion was the systematic minimization of stray light for the entire optical system. For exceptionally brilliant contrast and a new image quality with greater infor-mation content.The innovative simultaneous design process during optical modeling has resulted in a standardized opti-cal concept for all SteREO microscopes. For signifi-cantly improved resolution and a perceptibly betterThe Optical System: More Thanthe Sum of its Individual ComponentsToday, anyone developing a stereomicroscope that sets new standards with its optical system has to work constructively at the very limits of physical feasibility,taking full advantage of every new possibility offered by state-of-the-art optical design. With experience and innovativeness, you don’t have to look any further than the optical systems from Carl Zeiss.3 ranges of high-quality objectivesAchromat S: high-contrast images with a pronounced stereoscopic impression Plan S: flat,distortion-free object fieldsPlanApo S: precisely detailed resolution with no color fringes Parfocally harmonized for needle-sharp images over the entire magnification range from 1x to 8x: the new zoom body of SteREO Discovery.V8a.b.c.The Illumination: Show Your Specimen in a New Cold LightDesigned for slimline, space-saving light guides, opti-mized for flicker-free live images on the monitor,providing constant light output even if the line volt-age fluctuates, and with ventilation as quiet as a whisper – the high-intensity CL 1500 ECO cold lightThe quality of the illumination – this is all-important for contrasting in stereomicroscopy. The new fiber-optic CL 1500 ECO cold light source with its wide range of light guides and accessories offers you a variety of opportunities for highlighting your struc-tures perfectly.The fiber-optic CL 1500 ECO cold light source illuminates the specimen precisely with intensive infrared-free light.Here with a twin-arm goose neck for oblique reflected light with a targeted shadow effect.SMD-Board with white solder resist Reflected light with different light guides a.Linear slit light for lateral grazing light b.Fiber-optic annular slit illuminator for shadow-free 360°reflected lightc.Annular slit illuminator with polarization filter device to minimize reflective glare Objective: Plan S 1.0x Magnification: 15xContrasts with variable optimization in brightfield,darkfield and oblique light: the transmitted light equipment Ssource outperforms conventional fiber-optic systems thanks to several practical advantages, and offers excellent performance at a superb price!Incidentally, lamps and filters can be changed quick-ly and conveniently. Even when stacked.a.b.c.Or in a Completely Different Light: With White LEDsEach of the annular VisiLED illuminators is made up of eight LED segments that can be switched variably.A further advantage of noise-free light sources: upProviding the ability to change rapidly from shadow-free annular illumination to lateral oblique light, con-trast optimization through turning of oblique light around the specimen, continuous rotation of the illumi-nation for a stereoscopic impression of the object in the live image – and all this at the push of a button! The list of new contrasting possibilities offered by the VisiLED illumination system with its white LEDs is endless!The VisiLED HCT contrast stage offers a wide range of contrasts.It contains separate LED illuminators for brightfield and darkfield,and sliders for finely adjusta-ble oblique light.The LEDs are controlled using the MC1500 multicontroller.Mouth parts of the common houseflyTransmitted light with VisiLED HCT contrast stage a.Brightfieldteral darkfieldc.Oblique brightfield illumination Objective: PlanApo S 1.0x Magnification: 80xQuiet,durable and offering the best in daylight quality: VisiLED LED illuminationto 4 illumination settings can be stored and repro-duced again at any time.The MC1500 multicontroller of the VisiLED system allows control of reflected, transmitted and blended light.1.2.3.4.1. 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Better in position: the binocular ergo-phototube S 5-45°Ergonomics is also about choosing a relaxed sitting position when operating a microscope.The viewing angle and height have to coincide.The ergotube allows a free choice of viewing angle between 5 and 45 degrees.Intermediate tubes and two working positions for the eyepiece clamps vary the viewing height.4. Vertical 2D impression:the objective slideA must for documentation with subsequent image analysis,e.g.digital object measurements: the S/doc objective slide for the SteREO Discovery family of microscopes.Positioned directly beneath the zoom body,it enables the objective to be shifted precisely under one of the stereoscopic beam path for a vertical view of your specimen.The Expandable Platform:Flexible For a Variety of ApplicationsA typical feature of stereomicroscopes is their mod-ular system design. Equipped with intelligent inter-faces and fully integrated into the Carl Zeiss systems,SteREO Discovery.V8, with its comprehensive range of accessories, offers you a great deal of freedom in terms of organizing your workplace to suit your own practical needs.System OverviewSteREO Discovery.V8:The Technical DataObjectivesEyepiecesCarl Zeiss Microscopy GmbH 07745 Jena, Germany ********************www.zeiss.de/stereo-discoverye c t t o c h a n g e .e d o n e n v i r o n m e n t a l l y -f r i e n d l y r ,b l e a c h e d w i t h o u t t h e u s e o f r i n e .Instruments************************。
图像理解与计算机视觉
参考资料 – Google 讨论组 • Image Processing and Computer Vision – /group/ipcv – Google Scholar • – Google Search Engine – IEEE explorer – CVPR papers on the Web – ICCV papers on the Web – ECCV papers on the Web
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• ―UTokyo's e-Heritage Project: 3D Modeling of Heritage Sites‖
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一、教学目标与要求
目标:
《图像理解与计算机视觉》是一门涉及多个交叉学科领域的 课程。本课程侧重于图像理解和计算机视觉中的基本理论,课程 主要侧重对图像处理、目标识别以及计算机视觉方面的理论和应 用进行系统介绍。目标是使学生学习了本课程之后,对图像理解 和计算机视觉的基本理论,尤其是图像处理的概念、基本原理以 及解决问题的基本思想方法有一个较为全面的了解和领会;学习 计算机视觉的基本理论和技术,了解各种智能图像处理与计算机 视觉技术的相关应用;具备解决智能化检测与识别等应用问题的 初步能力,为以后从事模式识别、计算机视觉、测绘科学、多媒 体技术等领域的研究与工程建设打下扎实的基础
参考资料 – International Journal of Computer Vision (IJCV) – IEEE Transaction on Pattern Analysis and Machine Intelligence (TPAMI) – IEEE International Conference on Computer Vision and Pattern Recognition (CVPR) – IEEE Computer Society International Conference on Computer Vision (ICCV) – 其他国际期刊和会议论文: • Computer Vision and Image Understanding (CVIU) • Pattern Recognition Letters (PRL) • ECCV • ……
D-bar Sparks
4
A nice aspect of this theory is its natural presentation of Deligne cohomology in terms of forms and currents. In fact, we shall construct several different spark complexes, each yielding the same ring of spark classes containing Deligne cohomology. Hence, we also obtain several other geometric constructions of Deligne cohomology. k We note that the standard short exact sequence for the Deligne group HD (X, Z(p)) sits as the left column in our 3 × 3-grid. When X is compact Kaehler and k = 2p, this is 2p (X, Z(p)) → Hdgp,p (X ) → 0 where Jp (X ) is Griffiths’ the sequence: 0 → Jp (X ) → HD intermediate Jacobian. (See the diagrams following Proposition 14.4.) In our context it is trivial to see that every holomorphic cycle of codimension-p determines a class in 2p (X, Z(p)). Furthermore, one sees in a similar way that every maximally complex cycle HD 2p+1 (X, Z(p)), and if M bounds a M of codimension 2p + 1 determines a class [M ] ∈ HD holomorphic chain of (complex) codimension p, then [M ] = 0 (cf. Prop. 14.6). Recall that a powerful property of cohomology theory is its broad range of distinct formulations. Some presentations of the theory make it easy to compute, while others, such as de Rham theory, current theory or harmonic theory, lead to non-trivial assertions in analysis. Differential characters are similar in nature. There are many distinct formulations: some relatively simple and computable, and others rather more complicated, ˇ involving Cech-deRham complexes [19] or complexes of currents [20], [10], [14]. These latter approaches relate differential characters for example to refined characteristic classes for singular connections [16], [17], [22], to Morse Theory [18] and to harmonic theory. In [19] the homological apparatus of spark complexes was introduced to establish the equivalence of the many approaches to differential characters. In §1 below, that apparatus is generalized to treat a wide range of situations. In particular, on a complex manifold one can replace the deRham component of differential character theory by the ∂ -complex of (0, q )-forms, or more generally, the deRham complex truncated at level p. The machine developed in §1 is of independent interest and applies to a broad range of interesting situations. Using this machine we show that a variety of ∂ -spark complexes are equivalent and therefore lead to isomorphic groups of spark classes. Thus we are able to relate the classes ˇ double complex, of ∂ -gerbes with connection, which are defined within the Cech-Dolbeault to classes of currents satisfying a ∂ -spark equation of the form ∂a = φ − Ψ(R) where φ is a smooth ∂ -closed (0, q )-form and Ψ(R) is the (0, q )-component of a rectifiable cycle R of codimension q . These two are related by a larger enveloping complex which contains them both. Similar remarks apply to the case where one truncates at level p > 1. Other geometrically motivated spark complexes will be studied in forthcoming papers.
大学英语新视野3第三单元单词详解
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(2) prepare and use (land, soil, etc.) for growing crops 那里的大部分土地太贫瘠,无法耕种。 Most of the land there is too poor to cultivate. 他用一台大型拖拉机耕地。 He cultivated the field with a large tractor. 他退休以后就在家里种花,生活很舒适。 After he retired, he cultivated some flowers at home and he led a very comfortable life. 这里的人们主要种植稻子和豆类。 The people cultivate mainly rice and beans.
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Paragraph 3-11 5. spread: spread to: (cause to) reach sb. or sth. else, as by touching or other means of passing 消防队员成功地防止了火势蔓延到其他办公楼。 Firemen succeeded in preventing the fire from spreading to other office buildings. 这项运动已经发展到了牛津大学。 This movement spread to Oxford. 医生认为癌症已经扩散到了他的胃部,因此治疗起 来比较困难。 The doctor thought that the cancer has spread to his stomach, so it will be difficult to deal with.
CHAPTER I
CHAPTER IGLOBAL WEAK FORMS,WEIGHTED RESIDUALS,FINITE ELEMENTS,BOUNDARY ELEMENTS,&LOCAL WEAK FORMS1.1IntroductionDifferential equations(“ordinary differential equations”in one dimensional, and“partial differential equations”in two or three dimensional physical do-mains)and boundary conditions are abstract,and often highly approximate, characterizations of physical processes in engineering.In physical processes that evolve with time,derivatives with respect to time,and appropriate initial conditions,may also appear in these equations.Exact mathematical solutions are often possible only for problems defined in the simplest of geometrical domains,and only mostly for linear problems[i.e.,for differential equations and boundary/initial conditions wherein the unknown variable(s)and its(their) derivatives appear only in linear combinations.]However,most engineering processes occur mostly in complex geometrical domains,and most often,in-volve nonlinearities of the unknown variable(s)and its(their)derivatives.To solve such practical problems,to aid in engineering analysis,design,and syn-thesis,(digital)computer-based modeling&simulation techniques are neces-sary.We label this as“Computer-Modeling&Simulation-Based Engineering”. The aim is to use the power of the modern digital computer,high-speed sci-entific computing,visualization techniques,virtual reality,and the attendant information technologies,to achieve a near-real-time simulation of complex en-gineering phenomena,in order to facilitate integrated product&process design for real-life engineering systems.These include aircraft,spacecraft,missiles, automobiles,ships,power plants,bridges,biological systems,micro-electronic devices,computer chips,micro-electro-mechanical systems,systems involving heat and mass transfer,compressors,turbines,systems involvingfluidflow in closed and open domains,atmospheric polution,sustainable ecological tech-2Global Weak Forms,Weighted Residuals,Finite Elements,Boundary Elements,&Local Weak Forms nologies,nano,micro,meso and macro mechanics of engineered materials,etc. In as much as there is a great deal of commonality in the differential equations governing these processes,with appropriately defined unknown variable(s)gov-erning each process,one can envision a common“tool kit”that will enable com-puter modeling and simulation of a diverse variety of engineering processes.Engineering computations have made a startling progress over the past three decades.The most successful methods among them are thefinite element method and the boundary element method.However,as compared to its sound theoretical foundation,thefinite element method suffers from drawbacks such as locking(shear,membrane,incompressibility,etc),and tedious meshing or re-meshing in problems of crack propagation,shear-band formation,large de-formations,etc.Due to these reasons,in recent years,meshless approaches in solving the boundary value problems have received a considerable attention as new ways to alleviate some of these drawbacks.Meshless methods,as alternative numerical approaches to eliminate the well-known drawbacks in thefinite element and boundary element methods, have attracted much attention in recent decades,due to theirflexibility,and, most importantly,due to their potential in negating the need for the human-labor intensive process of constructing geometric meshes in a domain.Such meshless methods are especially useful in those problems with discontinuities or moving boundaries.The main objective of the meshless methods is to get rid of,or at least alleviate the difficulty of,meshing and remeshing the entire structure,by only adding or deleting nodes in the entire structure,instead.Meshless meth-ods may also alleviate some other problems associated with thefinite element method,such as locking,element distortion,and others.The initial idea of meshless methods dates back to the smooth particle hy-drodynamics(SPH)method for modeling astrophysical phenomena(Gingold and Monaghan,1977).The research into meshless methods has become very active,only after the publication of the Diffuse Element Method by Nayroles, Touzot&Villon(1992).Several so-called meshless methods[Element Free Galerkin(EFG)]by Belytschko,Lu&Gu(1994);Reproducing Kernel Particle Method(RKPM)by Liu,Chen,Uras&Chang(1996);the Partition of Unity Finite Element Method(PUFEM)by Babuska and Melenk(1997);hp-cloud method by Duarte and Oden1996;Natural Element Method(NEM)by Suku-mar,Moran&Belytschko(1998);Meshless Galerkin methods using Radial Basis Functions(RBF)by Wendland(1999);have also been reported in litera-1.1:Introduction3 ture since then.A detailed bibliography on meshless methods is provided at the end of this monograph.The major differences in these meshless methods come only from the techniques used for interpolating the trial function.Even though no mesh is required in these methods for the interpolation of the trial and test functions for the solution variables,the use of shadow elements is inevitable in these methods,for the integration of the weak-form,or of the energy.Therefore, these methods are not truly meshless.Recently,two truly meshless methods,the meshless local boundary inte-gral equation(LBIE)method,and the meshless local Petrov-Galerkin(MLPG) method,have been developed in Zhu,Zhang,&Atluri(1998a,b),Atluri&Zhu (1998a,b)and Atluri,Kim&Cho(1999),for solving linear and non-linear boundary problems.Both these methods are truly meshless,as no domain/or boundary meshes are required in these two approaches,either for the purposes of interpolation of the trial and test functions for the solution variables,or for the purposes of integration of the weak-form.All pertinent integrals can be easily evaluated over over-lapping,regularly shaped,domains(in general,spheres in three-dimensional problems)and their boundaries.In fact,The LBIE approach can be treated simply as a special case of the MLPG approach(Atluri,Kim, &Cho,1999).Zhang and Yao(2001)present a new regular hybrid boundary node method by combining the advantages of both LBIE and the boundary node method.Remarkable successes of the MLPG method have been reported in solving the convection-diffusion problems[Lin&Atluri(2000)];fracture me-chanics problems[Kim&Atluri(2000),Ching&Batra(2001)];Navier-Stokes flows[Lin&Atluri(2001)];Shear-deformable beams[Cho&Atluri(2001)]; and plate bending problems[Gu&Liu(2001),Long&Atluri(2002)],etc.In summary,the MLPG is a truly meshless method,which involves not only a meshless interpolation for the trial functions(such as MLS,PU,Shepard func-tion or RBF),but also a meshless integration of the weak-form(i.e.all integra-tions are always performed over regularly shaped sub-domains such as spheres, parallelopipeds,and ellipsoids in3-D).The aim of this monograph is an exposition of the MLPG method,in all its generality,and in all its variations.It is shown that some of the variations of the MLPG method not only eliminate the human-labor cost of meshing a domain altogether,but also involve less computational cost as compared to thefinite element and boundary element methods.4Global Weak Forms,Weighted Residuals,Finite Elements,Boundary Elements,&Local Weak Forms1.2Global weak forms and the weighted residual method(WRM) To set the stage for a discourse on the MLPG method,we start off by discussing a variety of modeling strategies,using Global Weak Forms,through an example problem.It can be shown that all mathematical formulations governing a variety of linear boundary value problems in engineering may be written in the form: L mΨf(1.1) where L m is a linear differential operator of order m.L m can be an“ordinary differential operator”in a one-dimensional problem,or a“partial differential operator”in2and3-dimensional physical domains.In a general3-D domain, imagine a line,going through the domain,and connecting two different points on the boundary.Along this line,one can imagine an ordinary differential equa-tion of order“m”.Then,at each point on the boundary,we may have m2 number of boundary conditions,each involving a differential operator of order m1.For example,we consider the linear Poisson’s equation in2-dimmensional space,defined by the Cartesian Coordinates x i.Consider the domainΩto be as sketched in Fig.1.1.The boundary ofΩ,denoted byΓ[or,sometimes, by∂Ω],is defined by the curve A-B-C-D-E-F-A,and the curve GH.Along the segment AB,the boundary conditionφφis prescribed.Like wise,the boundary conditions along the various segments are considered to be:∂φ∂n q along BC;φφand∂φ∂n q along parts of CD;∂φ∂n0along the slit (or“crack”)D-E-F;φφand∂φ∂n q along parts of FA;and∂φ∂n0 along the“hole”GH.The boundary value problem defined in Fig.1.1is a fairly realistic engineering problem.Hence,AB belongs to the essential boundaryΓu, and EF,ED and GH belong to theflux boundaryΓq.The Poisson equation can be can be written as:∇2φx p x xΩ(1.2)where x x i e i is the vector of position of a point insideΩ,p is a given source function,and the domainΩis enclosed byΓΓuΓq,with boundary condi-tions:φφonΓu(1.3a)∂φq q onΓq(1.3b)∂n1.2:Global weak forms and the weighted residual method(WRM)5Figure1.1:A realistic boundary value problem,∇2φx p x.The condition(1.3a)is often referred to as the Dirichlet boundary condition; and(1.3b)as the Neumann boundary condition.The Poisson equation arises in very many branches of engineering:the torsion of a solid rod of an arbitrary cross-section,undergoing an infinitesimal twist;heat transfer in homogeneous media;seepageflow;fluidfilm lubrication;eletro-staticfield;magneto-static field,etc.Let u,hereafter called the trial function,be an approximate solution to the problem(1.2).In as much as u may not be an exact solution,substituting u in the differential equation and the boundary conditions Eqs.(1.2-1.3),we obtain the following relations for the“error residuals”.Interior Error:R I x∇2u x p x0(1.4)Boundary Error:R B1u x u0atΓuR B2∂u∂nq atΓq(1.5)6Global Weak Forms,Weighted Residuals,Finite Elements,Boundary Elements,&Local Weak Formswhere R I is the interior error;and R Bii12are the errors in the boundary conditions.The“best”approximation is the one that nullifies the errors R I and R Biin some fashion.In general,the trial functions must satisfy several minimum re-quirements to make the process of error nullification meaningful.The functions that satisfy such minimum requirements are called the admissible functions.For example,in Eq.(1.4),u must be2times differentiable and u i must be contin-uous(or u is C1continuous);if u is not C1continuous,u ii will be“infinite”where u i is discontinuous.In that case,R I u is infinite at these points;and the minimization of R I u no longer makes any sense.Consider a linear combination of N admissible functions u i(i12N), such that:uN∑i1a i u i x a i u i x(1.6)where a i(i12N)are undetermined coefficients.We use the convention that summation is implied over a repeated index.Here,choosing an admissible u x[i.e.,C1continuous u x in Eq.(1.4)]over a global domainΩ,of arbitrary shape is a non-trivial proposition.Much of Chapter2in this monograph is devoted to this topic.However,ifΩis a simple geometry,such as a circle, square,etc.,u x can be in the form of trigonometric or other functions.Figure1.2:Schematics of the point collocation methodWe now discuss several methods,to reduce the errors R I and R Bito be as1.2:Global weak forms and the weighted residual method(WRM)7 small as possible,and in the limit,make them uniformly zero over the globaldomainΩ.1.2.1Point collocation methodWe assume that u is C1continuous all overΩin Eq.(1.4).We consider making the error vanish at certain points x j j12M,in the domainΩ.This leads to the following equations for the undetermined coefficients.R I x j a i∇2u i x j p x j0j12M(1.7) andR Bix j0i12(1.8) Suppose that we use the conditions of vanishing of the two types of boundary residuals[Eq.(1.8)]to generate N M equations;then,by using M collocation points in the interior of the domainΩ,we can generate N equations for the N undetermined coefficients a i.While a solution a j for such a system of equationswill make the errors R I and R Bigo to zero identically at afinite number of points,the residuals R I and R Bimay oscillate in between these points and may indeed be quite ing more collocation points than M will result in more equations than the unknowns.In this case,it is not possible,in general,tofind a set of coefficients a i that will drive the error at the collocation points to zero.Suppose that point collocation of Eqs.(1.7)at an arbitrarily large number of points,along with enforcing(1.8)at an arbitrary number of points,lead,in general,to the over-determined system of equations:A i j a j p i(1.9) where i12K;j12N and K N.We seek an approximate solu-tion a j for a j,such thatA i j a j p iεi0(1.10) and a j minimize the square error,εiεi.Thus,∂∂a j εiεi∂∂a j A ip a pp i A iq a q p i0(1.11)8Global Weak Forms,Weighted Residuals,Finite Elements,Boundary Elements,&Local Weak FormsorA i j A iq a q A i j p i(1.12) orB jq a q p i(1.13) where i12K;j12K and q12N.The above method is an algebraic least-squares procedure to approximately solve an over-determined system of equations,provided that B jq is positive def-inite.For an underdetermined system of equations,however,only some of the unknowns can be expressed in terms of the other unknowns.It is noted that Eq.(1.11)also amounts to minimizing the summed point-wise square error. 1.2.2Weighted integral square errorAs discussed above,in the point collocation method,we can use more colloca-tion points than the number of unknown coefficients in the trial function,using a least square error approach.In the limit,as the number of collocation points tends to∞,we may consider minimizing the integrated square error:εσΩ∇2u x p x2dΩβΓuu u2dΓγΓq∂u∂nq2dΓ(1.14)whereσ,β,γare weighting constants,which are also often referred to as “penalty-parameters”.By minimizing the aboveεwith respect to a i,one may obtain the desired system of N algebraic equations to determine the N unknownsa i.1.2.3Subdomain integral/average error methodAlternatively,we may consider making each of the averages of the error,over a set of subdomains,go to zero.For example,we may setΩk R i x dΩ0;∂ΩkR i x dΓ0(1.15)The number of subdomains is chosen such that we have a solvable set of equa-tions for a i,i12N[i.e.N,or more than N subdomains,to yield a1.2:Global weak forms and the weighted residual method(WRM)9 system of N equations,or of more than N equations].This is illustrated in Fig.1.3.Note that the subdomainsΩi i12k are continguous(i.e.,non-overlapping),and span the entire domainΩ.While most ofΩi may be of a regular[say triangular]shape,others may be approximately triangular.Figure1.3:Schematics of the subdomains1.2.4Finite volume methodThis is similar to the Subdomain Integral method,and has been popularized in the literature dealing with unsteady aerodynamics,and heat transfer.The prin-ciple of thefinite volume scheme is to integrate Eq.(1.2)on a control volume (i.e.subdomain)Ωk,which yields:∂Ωk u i n i dΓΩkpdΩ0(1.16)where∂Ωk is the boundary of the subdomainΩk,andΩkΩ;next,thefluxes need to be approximated on the boundary∂Ωk of the control volume.Hence, we shall approximate the integral of u i n i over each edge of the mesh.Note, once again,that the sub-domainsΩk are contiguous,as in Fig.1.3.10Global Weak Forms,Weighted Residuals,Finite Elements,Boundary Elements,&Local Weak Forms Another variant of the Finite V olume Method may be derived,by rewriting Eq.(1.2)in a“mixed”form:φiφi;φi i p(1.17) wherein,φandφi are treated as independent variables.If u and u i are the trial functions forφandφi,respectively,we may write the counterparts of(1.16)as:∂Ωk un i dΓΩku i dΩ0(1.18)and∂Ωk u i n i dΓΩkpdΩ0(1.19)Instead of the“global trial function”,u a k u k x;and u i a k u ki x,one may assume a linear interpolation of u and u i over each element,as shown in Fig.1.3.Note again,all the subdomainsΩk are contiguous in Fig. 1.3,and the method involves the generation of a“mesh”,for both the purpose of interpola-tion,as well as for purpose of integration,as in Eqs.(1.18)and(1.19)]1.2.5The weighted residual method and global weak formsIf the function F x satisfies the conditionΩF x g x dΩ0(1.20) for all g x onΩ,then,F x0onΩ.Conversely,therefore,we canfind the trial function u a i u i such that R I u0[where R I is defined in Eq.(1.7)] by enforcing the weak form equationΩR I x v x dΩ0(1.21) for all possible functions v x onΩ.We denote v x as“test”functions.In general,the trial function u x is chosen to be a linear combination of a set of basis functions,u i(i12N),with undetermined coefficients,a i,i.e. u a i u i x,xΩ.Likewise,the test function v x is chosen as v b j v j x, j12M;where v j are the basis functions and b j are the undetermined1.2:Global weak forms and the weighted residual method(WRM)11 coefficients.The“best”approximation is obtained by determining that combi-nation of u i that satisfies the weak form equation(1.21)for the chosen test func-tions v j.Different choices of the basis functions for the trial function and the test functions will lead to different approximation methods.For example,it reduces to the Point Collocation Method when Dirac Delta functions,v xδx x j, are used for the test functions.It reduces to the subdomain integral method, when the following piecewise constant functions[or Heaviside step functions] are used as test functions:v x1xΩk[see Fig.1.3]0elsewhere(1.22)When the test function v x is taken to be the same as the error function R I, Eq.(1.21)reduces to the least square error method.Now,consider the weighted interior residual equation for the Poisson’s prob-lem,governed by Eq.(1.2):Ω∇2u x p x v x dΩ0(1.23)which requires u to be twice differentiable and u i to be continuous[or u is C1 continuous].If not,u ii will be∞where u i is discontinuous and(1.23)makes no sense.On the other hand,there is no continuity requirement on the test function v in Eq.(1.23).Thus,the requirements on u and v are“unsymmetric”, in order to be admissible in Eq.(1.23).Hence,we denote Eq.(1.23)as a global unsymmetric weak form(GUSWF).To reduce this high-order differentiability requirement on u,we can inte-grate Eq.(1.23)by parts,by using∇2u v u ii v u i v i u i v i,to obtain the following global symmetric weak formulation(GSWF),Γu i n i vdΓΩu i v i pv dΩ0(1.24)which has the same differentiability requirements on both the trial function u and the test function v in the interior of the domainΩ,namely,both u and v are required to be once differentiable,and both u and v are required to be C0continuous.If they are not C0continuous,u i and v i may tend to∞when u and v are discontinuous and Eq.(1.24)is no longer meaningful.Thus,the12Global Weak Forms,Weighted Residuals,Finite Elements,Boundary Elements,&Local Weak Forms requirement on the test function is“increased”,while the requirement on the trial function is“decreased”.We may directly substitute the natural boundary condition Eq.(1.3b)into the symmetric weak form equation,i.e.Eq.(1.24),and noticing that u i n i∂u∂n q in Eq.(1.24),we obtainΓu u i n i vdΓΓqqvdΓΩu i v i pv dΩ0(1.25)When all the boundary conditions are natural,(or“Generalized Force”type), we may rewrite Eq.(1.25)asΓq qvdΓΩu i v i pv dΩ0(1.26)We can see that Eq.(1.26)is actually the combined weak form equation for both the differential equation(D.E.)and the boundary conditions(B.C.),if these B.C. are purely of the“natural”or“kinetic”,or“generalized-force”type.Let u be approximated using u i(i12N),i.e.u a i u i i12N(1.27)where a i are undermined coefficients.Note that,in order to be admissible,u i need only to be C0continuous in the domainΩ,,but they need not obey any boundary conditions a priori,in as much as the boundary condition for u,if they are of the“natural”or“kinetic”type,i.e.,Eq.(1.3b),is already embedded in the weak form Eq.(1.26).Let v be any function that can be represented asv b j v j j12M(1.28)where b i are arbitrary constants.Note again,that in as much as the prescribed boundary conditions for u are purely natural as in Eq.(1.3b),the test func-tion v need not obey any boundary conditions,as seen from Eq.(1.26).Using Eqs.(1.27)and(1.28)in Eq.(1.26),we obtainΓq qb j v j dΓΩa i u i kb j v j k pb j v j dΩ0(1.29)Since Eq.(1.29)is true for any b j,we have the following linear system of equa-tions for a i.A i j a i f j(1.30)1.2:Global weak forms and the weighted residual method(WRM)13 where i12N;j12M,andA i jΩu i k v j k dΩ(1.31)f jΩpv j dΩΓqqv j dΓ(1.32)If M N[i.e.,the number of basis functions in the trial function u,is the same as the number of basis functions in the test function v],and u j are identically the same as v j j12N,we have a symmetric A i j.When v j u j,the method is generally known as the Galerkin symmetric weak form approach.When the test functions v j are in general different from u j,the method is known as the Petrov-Galerkin approach.In this case,even when M N and even when a symmetric weak form is used,the coefficient matrix A i j is unsymmetric.When M N,the system of Eq.(1.30)is over-determined,and can be solved by the method of algebraic least squares.Also,when m n,and u j v j,the coefficient matrix A i j in Eq.(1.30)is symmetric and positive definite,as long as“rigid body modes”[i.e.u j is a constant or linear function],are removed.Suppose now that the B.C.are purely kinematic[i.e.,ΓΓu],i.e.essen-tial boundary condition Eq.(1.3a)exists all over the boundary.If we examine the GSWF(1.24),we notice that the above“lower-order”or purely“kinematic”B.C.(1.3a)cannot be directly substituted into the GSWF(1.24).Unless we choose to add additional terms to Eq.(1.24)to enforce essential boundary con-dition(1.3a)in a weak form,we must choose the trial function u to satisfy these conditions(1.3a)identically,a priori.In this case,we are left with the GSWF (1.24)with boundary terms as indicated in Eq.(1.24).We can eliminate these boundary terms onΓin Eq.(1.24),if we choose the test functions such that v x0,xΓ.If,on the otherhand,in the case when the boundary conditions are entirely kinematic,i.e.,only on u,and if,correspondingly,v does not vanish at the boundary,we have the discrete weak form(similar to1.29)as:Γa i u i k n k b j v j dΓΩa i u i kb j v j k pb j v j dΩ0(1.33)leading to the discrete equation A i j a j f i,whereA i jΩu i k v j k dΩΓu i k n k v j dΓ(1.34a)and f jΩpv j dΩ(1.34b)14Global Weak Forms,Weighted Residuals,Finite Elements,Boundary Elements,&Local Weak Forms It is seen that nothing can be said of the positive definiteness of A i j in (1.34a),which does not assure the solvability of the problem.On the other-hand,if v j vanish at the boundary,A i j reduces to that in Eq.(1.31),which is positive definite(when rigid modes are suppressed).Hence a solution always exists for a i.Thus,if the given problem has prescribed boundary conditions that are purely of the kinematic type,i.e.,as in Eq.(1.3a)[i.e.,ΓΓu],we choose u to obey these conditions a priori,and correspondingly choose v such that v x0,xΓ.In this case,the GSWF reduces to:Ωu i v i pv dΩ0(1.35)when all the B.C.are purely kinematic.If the trial function u,especially in2and3-dimensional problems,cannot be chosen so as to satisfy the essential boundary conditions a priori,one can enforce them by:(i)choosing a boundary weighting function that may depend on the higher-order derivatives of the test function v,such that the kinematic boundary conditions are enforced by the weak-form:Γuu u v i n i dΓ0(1.36)However,when the bilinear form arising out ofΓu uv i n i dΓis added to the A i jin Eq.(1.34b),the positive definiteness of the resulting coefficient matrix A i j cannot be guaranteed;(ii)by choosing an independent Lagrange multiplierfield at the boundary[this is also not desirable,since the solvability of the problem will involve certain stability conditions which must be satisfied a priori[Brezzi (1974)];(iii)by using boundary collocation for the essential B.C.at a desired number of points;(iv)by using the least-squares integral error condition for boundary error residuals;or(v)by using a“Penalty”approach.Methods(iii)to (v)are in general simpler than the others.More will be said of these essential boundary conditions,and their satisfaction,later in this book,in the context of meshless methods.In general,in the GSWF(1.24),one can directly substitute any higher-order B.C.(natural)into(1.24),and thus enforce them a posteriori;while all lower-order(essential)B.C.must be satisfied a priori,and the GSWF is then simpli-fied by enforcing v to satisfy the homogeneous condition atΓu.1.2:Global weak forms and the weighted residual method(WRM)15Now,we use the formalism that the test function v is considered to be a “variation”of the trial function u,in the traditional“calculus of variations”sense.For,example,in general,if L2m is a self-adjoint operator,i.e.L2m u vdΩL m v L m u dΩB(1.37) where B are boundary integral terms,then aπexist so thatδπ0leads to L2m u p,whereπ12L m u2pu dΩB(1.38) In a elastic system with a conservative(dead-load)forces,πis the“Total Po-tential Energy”,andδπ0is the condition of stationarity of the total potential energy.It may simply be viewed as a mathematical equivalent of the symmetric weak form,which,however,is more direct.In general,the weak form approach is,however,more general than the above“energy approach”,in as much as a weak form can be stated for non-self-adjoint operators as well.The Galerkin Finite Element Method(GFEM)is based on the Global Symmetric Weak Form (GSWF),Eq.(1.24).To reduce the C0continuity conditions as demanded by the Symmetric Weak form(1.24),we can integrate Eq.(1.23)by parts twice,by using∇2u vu ii v u i v i uv i i uv ii,to obtain another global unsymmetric weak for-mulation(GUSWF)as follows,Γu i n i vdΓΓuv i n i dΓΩu∇2v pv dΩ0(1.39)which requires the test function v to be twice differentiable and v i to be contin-uous[or v is C1continuous].If not,v ii will be∞where v i is discontinuous and (1.39)makes no sense.On the other hand,there is no continuity requirement on the trial function u in Eq.(1.39).Thus,the requirements on u and v are also “unsymmetric”,in order to be admissible in Eq.(1.39).Hence,we also denote Eq.(1.39)as a global unsymmetric weak form(GUSWF2).In this case,we may directly substitute the natrural and essential bound-ary conditions Eqs.(1.3a)and(1.3b)into the global unsymmetric weak form equation,i.e.Eq.(1.39),we obtainΓu qvdΓΓqqvdΓΓuuv i n i dΓΓquv i n i dΓΩu∇2v pv dΩ0(1.40)16Global Weak Forms,Weighted Residuals,Finite Elements,Boundary Elements,&Local Weak Forms1.3The Galerkinfinite element methodIn the previous section,the basis functions u j and v j for the trial function u and the test function v,were at once assumed as“global”functions,and each of it was nonzero over the entire problem-domain,Ω.Figure1.4:Use of a patch work of generic triangular elements to approximate the given geometry in Fig.1.1In a one-dimensional problem,assuming component trial and test functions u j and v j over the entire problem-domain is relatively simple.On the other hand,if the problem is defined by a partial differential equation in2or3dimen-sions,and if the global domain is of an arbitrary shape,assuming the trial and test functions as simple polynomials over the entire global domain is inconve-nient at best.To overcome this curse of arbitrary shaped geometrical domains wherein the problem is defined,one may resort to assuming trial and test func-tions over a generic simpler-shaped subdomain(element)of the given problem, and create a non-overlapping patchwork of the subdomains(elements)to geo-metrically approximate the given domain(see Fig.1.4).We can assume the trial and test functions over each subdomain(element)as“local basis”or“element basis”functions.。
EM-30系列双目立体镜与变倍镜指南说明书
Table of Contents1) Introduction2-3) Construction of the microscope 4-5) Functions of the microscope 6) Preparing the microscope for use 7-9) Working with the microscope 10-11) Maintenance and cleaningIntroductionWith your purchase of a EM-30 (zoom) stereo microscope you have chosen for a quality product. The EM-30 is developed for use at schools, and by collectors of minerals, stamps etc.The stereo microscope consists of two separate microscope tubes which are combined as a unit, in order to focus them simultaneously on the object. Each tube has prisms, achromatic objectives and a widefield eyepiece in order to obtain a large, flat field of view. Both eyes are looking at the object under a different angle to reach a deep stereoscopic image.The maintenance requirement is limited when using the microscope in a decent manner.This manual describes the construction of the microscope, how to use the microscope and maintenance of the microscope.Construction of the Microscope The names of the several parts are listed below andare indicated in the picture on the next page:A) Photo tube with focussing (trinocular models)B) Carrying HandleC) Connector indicdent illuminatorD) Focusing knob(s)E) Intensity controller for incident illuminationF) Stand foot with transmitted illuminationG) EyepieceH) Diopter correctionI) Prism housingJ) Zoom knob(s)K) Objective cover / revolverL) Incident illuminationM) Intensity controller transmitted illumination N) Object clipO) Object plateA C D E F G H IK LOFunctions of the MicroscopeThe stereo microscope consists of a stand with holder/focusing system, in which the stereo head is placed and locked with set screw .Always hold the microscope at its arm and grip when moving it.TubeThe zoom stereo microscope heads of the EM-30 are equipped with a 45 degrees tube, which is rotatable over 360 degrees. Each type has a diopter adjustment ring on both eyepiece tubes.Optical specifications of the MT-30/MT-90 series rangeThe zoom stereo microscopes of the EM-30 are equipped with 2 zoom objectives and a pair of wide field WF10x eyepieces. The stereo microscopes of the EM-30 are equipped with a revolving nosepiece in which 2 pairs of achromatic objectives are mounted, and a wide field WF10x pair of eyepieces. In the tabel below some available models are listed.Eyepieces Objectives Magnifications Execution TubeWF10x1x / 3x10x / 30x binocular45 degreesWF10x2x / 4x20x / 40x binocular45 degreesWF10x0.7x ~ 4.5x7x ~ 45x binocular45 degreesWF10x0.7x ~ 4.5x7x ~ 45x trinocular45 degrees10x100x1000xObject stageThe stand is equipped with an object stage with a semi transparent stage plate (O) and 2 object clips (N).FocusingWith the focusing knobs (D) the object can be sharply focussed.Magnification adjustmentThe zoom stereo microscopes of the EM-30 are equipped with 2 achromatic zoom objectives. By using the zoom knobs (J) the magnification can be adjusted in a smooth, stepless way. Magnification adjustmentThe stereo versions(1/3x or 2/4x) are equipped with 2 pairs of achromatic objectives in a revolving nosepiece (K). By rotating this nosepiece over 180 degrees another magnification is set. Turn the nosepiece untill it clearly “clicks” into position.IlluminationThe stand is equipped with transmitted and incident LED illumination of 3 Watt. The illuminators can be used simultaneously. On the side of the foot the transmitted light intensity can be adjusted with a small wheel (M) (not visible in the picture). At the back of the base the Intensity controller for incident illumination can be found (E).Preparing the Microscope for Use Take the stereo microscope out of its packing and putit on a firm stable table. Connect the power cable to the mains supply and switch on the microscope. Place the eyeshades onto the eyepieces. Sit comfortably down behind the microscope and take a relaxed po-sition while viewing through the eyepieces (G). The third (photo) tube of the trinocular models is packed in the lid of the styrofoam packing. Take it out and place it onto the microscope.Working with the Microscope• Place an object onto the stage plate and adjust the height of the holder randomly with the focussing knobs (D) at the backside of the stand.• Set both diopter adjustment rings(H) to the “O” position• Adjust the interpupillary distance by moving both prism housings (I) towards each other until one round image is seen with both eyes.Setting the eyepieces in order to have a sharp image over the complete zoom range• Set the magnification at the highest position by means of the zoom knob (J) and sharply focus on a flat specimen.• Now bring the magnification down to the lowest position.• First correct the sharpness with only the left hand diopter adjustment ring (H), and than for the right hand one.Photo and videoTaking pictures with an normal or digital SLR camera with the trinocular zoom types is done with the help of microscope adapter set (optional).One can adjust the height of the tube of the trinocular models by turning the ring of the tube in order to reach the same focus point between the the eyepieces and the photo tube. For showing images on a monitor or PC, by means of a CCD or CMOS camera, one needs an optional C-mount adapter . Having the same focal point between eyepieces and the screen is reached by following above mentioned procedure.。
南昌2024年07版小学4年级上册第十一次英语第6单元测验卷
南昌2024年07版小学4年级上册英语第6单元测验卷考试时间:90分钟(总分:120)A卷考试人:_________题号一二三总分得分一、选择题(共计20题,共40分)1、What does "植物网络" mean in English?A, Plant networkB, Agricultural networkC, Environmental networkD, Ecological network2、Where do fish live?鱼生活在哪里?A. In the sky 天空B. In the water 水中C. On land 陆地上D. In trees 树上3、What do you call the time when the sun rises?A, MorningB, NoonC, EveningD, Night4、Which plant is often used as a garden decoration?哪种植物常用作花园装饰?A. Flowering plant (开花植物)B. Grass (草)C. Oak (橡树)D. Pine (松树)5、Which animal is famous for its ability to survive extremetemperatures?哪种动物以能在极端温度下生存而闻名?A) Arctic Fox (北极狐)B) Camel (骆驼)C) Both (两者)D) None of the above (以上皆不是)6、What is the name of the famous scientist who developed the theory of evolution?提出进化论的著名科学家叫什么名字?A) Charles Darwin / 查尔斯·达尔文B. Gregor Mendel / 格雷戈尔·孟德尔C. Louis Pasteur / 路易·巴斯德D. Albert Einstein / 阿尔伯特·爱因斯坦7、Which fruit is yellow?A, AppleB, BananaC, GrapeD, Orange8、What do you call a young horse?小马叫什么?A) FoalB) CalfC) KidD) Pup9、How do you say "我在这里" in English?A, I'm happyB, I'm hereC, I'm thereD, I'm gone10、What color is the sky on a clear day?A, GreenB, BlueC, YellowD, Red11、你喜欢什么职业?What job do you like?A. 医生 (Doctor)B. 教师 (Teacher)C. 工程师 (Engineer)D. 艺术家 (Artist)12、Which animal is known for its ability to climbmountains?哪种动物以其爬山能力而闻名?A) GoatB) SheepC) LynxD) All of the above13、What is the name of the tree that produces acorns?A, PineB, MapleC, Oak14、Where _____ you live?A, DoB, DoesC, IsD, Are15、What do you call a type of visual art?你称一种视觉艺术为?A. Visual ArtB. Graphic ArtC. Decorative ArtD. All of the above16、What do you call a young camel?小骆驼叫什么?A) CalfB) FoalC) KidD) Pup17、Which type of plant reproduces by spores?哪种植物通过孢子繁殖?A, FernB, OakC, CactusD, Grass18、Where do we go to learn?中文解释:我们去哪里学习?A, ParkB, SchoolC, Store19、Which animal can be found in the Arctic?哪种动物可以在北极找到?A) Polar bearB) PenguinC) SealD) All of the above20、What do you call the area where a football game is played?足球比赛进行的区域称为何?A. Court 法庭B. Field 球场C. Arena 圆形剧场D. Ring 拳击场二、听力题(共计20题,共40分)1、听力填空题:She ___ (not/visit) her cousins last summer.2、What food do we usually eat for breakfast?A, PizzaB, CerealC, PastaD, Burger3、听力填空题(传统文化)Every culture has its own unique traditions. In my culture, we celebrate the _____ Festival, where we eat mooncakes and admire the full moon. It is a time for family reunions and _____ together. I look forward to it every year!4、What do we call the food made from ground meat?A, SausageB, SteakC, BurgerD, Kebab5、听力填空题:He ___ (not/like) to read mystery books.6、听力填空题(美丽的自然)Nature is full of wonders. From tall mountains to deep _____, every part of nature is unique. Spending time outdoors helps us relax and appreciate the beauty of our surroundings.7、听力填空题:They ___ (not/play) outside when it snows.8、听力填空题:The birds ___ (sing) in the morning.9、What do you need to start a fire?A, WaterB, WoodC, IceD, Dirt10、听力填空题:The main source of energy for plants is ______.11、听力朗读。
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are valid and have the highest correlation total. In the following sections we describe the two algorithms in detail and experimentally demonstrate and compare their results.
Proc. International Conference on Pattern Recognition (ICPR’00), Vol 1, pp 567-570, 2000.
1
Trinocular Stereo for Non-Parallel Configurations
Jane Mulligan and Kostas Daniilidis GRASP Laboratory, University of Pennsylvania, Philadelphia, PA, USA Abstract
2. Full Calculation
We begin by independently rectifying the left and centre cameras (L and CL ) and the centre and right cameras ( CR and R), so that their epipolar lines are parallel respectively. For the right rectified camera pair every disparity dR to be searched represents a plane with constant Z , which can be projected into the L and CL images to compute the corresponding uL ; vL ; dL ] for each uR ; vR ; dR ]. This straightforward application of the trinocular constraint is illustrated in Figure 1. Of course for any Z -plane constructed from dR , a range of dL will be required to match points in the left pair. For example for the images used later, the right range DR = ?90; 10] corresponds to a left range DL = ?74; 67]. Also because the two pairs are independently rectified, corresponding points in the left pair will not necessarily have vL = vR , thus all of uL, vL , and dL depend on uR ; vR ; dR ]. The calculation is simplified slightly by the fact that CL and CR are derived from the same image C and are related by the a priori rectification rotations RCL and RCR . We can thus precompute a lookup table of locations in CL equivalent to those in CR by precalculating uCL ; vCL ; s] = ?1 uCR ; vCR ; 1]T , for all image locations. RCLRCR Our underlying matching measure is modified normalized cross correlation (MNCC) of the form: MNCC =
C
CL
Figure 1. Trinocular camera triple. The configurations we are interested in are similar to that depicted in Figure 1, where a sequence of cameras surrounds an object to be modeled or a user interacting with an augmented reality system. To obtain the accuracy we require for these tasks as well as facilitate merging and registering of multiple views, we use a fixed strongly calibrated camera rig. To generate dense accurate depth maps in such a scenario we implemented 2 trinocular stereo algorithms. Both treat the cameras as 2 independent pairs, left and centre and centre and right. The first algorithm combines correlation values from the two pairs by precomputing correlation images for ranges of disparity in the left camera pair, then the computed correlation for each tested uR ; vR ; dR ] is added to that precomputed for the corresponding uL ; vL ; dL ]. This results in large correlation lookup tables for the left image pair. As an alternative we tested an algorithm which computes correlations over a range of disparities independently for both image pairs. It retains only the N highest correlation values for each location in each pair. Much like the edge match hypotheses from the literature, these can be cross checked to see which
dr
L bL
CR
R bR
1. Introduction
Reconstructions from a single stereo pair often have errors and extreme outliers due to ambiguity in matches along the epipolar line. For applications such as building detailed object models or creating models of humans for virtual environments, identifying and eliminating such points or patches is critical, but often difficult and expensive. One well known constraint for reducing these ambiguities is to add a third camera to verify hypothesized matches. However, most trinocular systems proposed in the literature exploit a right triangular [5, 1, 3, 4] and/or parallel [6] camera triple configuration. The close range scanning tasks we are interested in are better served by a surround configuration of cameras, which disallows the triple rectification methods which simplify these parallel camera approaches. The trinocular epipolar constraint in stereo vision is based on the fact that for a hypothesized match u; v; d] in a pair of images, there is a unique location we can predict in the third camera image where we expect to find evidence of the same world point [2]. A hypothesis is correct if the epipolar lines in the third camera image for the original point u; v ] and the hypothesized match u ? d; v ], intersect. For edge based systems this means checking a series of rel-