Wavelength assignment in optical networks with fixed fiber capacity
弹性光网络中路由与频谱分配算法综述
第44卷 第6期系统工程与电子技术Vol.44 No.62022年6月SystemsEngineering andElectronicsJune2022文章编号:1001 506X(2022)06 2001 10 网址:www.sys ele.com收稿日期:20210517;修回日期:20210918;网络优先出版日期:20211225。
网络优先出版地址:https:∥kns.cnki.net/kcms/detail/11.2422.TN.20211225.1902.002.html基金项目:陕西省自然科学基础研究计划(2021JQ 380)资助课题 通讯作者.引用格式:张佳唯,钱凤臣,杨俊强,等.弹性光网络中路由与频谱分配算法综述[J].系统工程与电子技术,2022,44(6):2001 2010.犚犲犳犲狉犲狀犮犲犳狅狉犿犪狋:ZHANGJW,QIANFC,YANGJQ,etal.Surveyonroutingandspectrumallocationalgorithminelasticopticalnetworks[J].SystemsEngineeringandElectronics,2022,44(6):2001 2010.弹性光网络中路由与频谱分配算法综述张佳唯 ,钱凤臣,杨俊强,赵 骞,张峥嵘(国防科技大学信息通信学院,陕西西安710106) 摘 要:弹性光网络(elasticopticalnetworks,EONs)作为下一代极具潜力的光网络近年来受到广泛关注,其中路由与频谱分配(routingandspectrumallocation,RSA)是实现网络设计和控制的核心技术之一。
本文系统分析了EONs的概念内涵,对RSA这一关键问题进行了详细描述,从静态和动态角度出发,以不同特性的算法框架为基础,依照精确算法、智能优化算法、启发式算法以及学习型算法4个大类对RSA算法的国内外研究现状进行了总结剖析。
光电子材料导论第一章 信息处理技术和材料-全光波长转换 (2)-PPT精品文档22页
Long SOA has superior dynamic performance
Long SOA only has 30 nm bandwidth, whereas it is 60 nm for short SOA.
Smaller bandwidth gives larger differential gain at the short wavelength side of the gain peak, a larger extinction ratio of the converted signal is expected for the long SOA
Wavelength conversion is a very useful function in advanced optical systems.
The converters should feature the followings: •Bit-rate transparency (up to at least 10 Gb/s). •No extinction ratio degradation. •high signal-to-noise ratio at the output (to ensure cascad-ability) •Moderate input power levels(~0 dBm).
• Large wavelength span for both input and output signals.
• Possibility for same input and output wavelengths (no conversion).
DWDM波长路由网络光链路负载均衡的波长路由算法
信息光电子DWDM波长路由网络光链路负载均衡的波长路由算法*李 蔚**,何 军,刘德明,黄德修(华中科技大学光电子工程系,湖北武汉430074)摘要:提出了一种应用于密集波分复用(DWD M)波长路由网络(WRON)中光链路负荷均衡的思想,并将其应用于优化Dijks tra算法的权值,同时将优化Dijkstra算法用于遗传算法求得了在不同的负荷条件下波长下限的网络所需波长数目。
并将优化前后的算法分别对美国自然科学基金(NSF)网络的最优波长分配进行数值分析,发现基于负荷均衡思想的优化Dijkstra算法能够对网络的性能有很大提高:当遗传代数为20代时,采用优化Dijkstra算法阻塞率降低了约36%;当波长使用数为7个时,降低网络阻塞率10%。
关键词:波长路由网络(WRON);路由波长分配(RWA);光链路负荷均衡;优化Dijkstra算法;遗传算法;阻塞率中图分类号:TN913 文献标识码:A 文章编号:1005 0086(2004)02 0173 05Wavelength Assignment Algorithm with Load Balance in a DWDM WRONLI Wei**,HE Jun,LIU De ming,HUANG De xiu(Department of Op toelectronic Engineering,Huazhong University of Science and Technology,Wuhan430074,China)Abstract:A new m ethod of balancing the optical path load was presented for optimizing the wei ght of Dijks traalgorithm in a DWDM wavelength routi ng optical networks(WRON).Thi s optimized D ijkstra algorithm wasapplied in the genetic algorithm to obtain the minimal wavelength num ber under the different path load conditi on.The optimal wavelength number in the national science fund(NSF)networks of USA was us ing this opti m ized and common Dijks tra algorithm,respectively.The num erical com puting result shows that the perform ance of the blocki ng probability has been improved greatly.The blocking probability can be reduce36%and10%respectively when the genetic generati on i s20and the num ber of wavelength is7.Key w ords:wavelength routing optical networks(WRON);routering and wavelength ass ignment(RW A);optical path load balance;optim i z ed D ijkstra algorithm;genetic algorithm;blocking probability1 引 言随着密集波分复用(DW DM)网络的拓扑结构从点到点向多光纤Mesh格形网络的演变,DW DM波长路由网络(WRON)得到越来越多的应用。
光纤环形谐振腔英文
光纤环形谐振腔英文Fiber Optic Ring Resonator.Fiber optic ring resonators have emerged as a crucial component in modern optical systems, offering unique capabilities for controlling and manipulating light. These resonators consist of a closed loop of optical fiber that supports light propagation in a circular path, enabling light to build up and interfere within the cavity. This interference leads to the formation of resonant modes, which are characterized by specific wavelengths of light that experience enhanced transmission or reflection.The fundamental operation of a fiber optic ring resonator relies on the principles of waveguide optics and interference. Light introduced into the resonator couples into the closed loop and propagates around the ring, experiencing phase shifts and intensity variations as it traverses the cavity. The length of the resonator determines the resonant frequencies, and the refractiveindex of the waveguide material affects the phase velocity of the light.One of the key advantages of fiber optic ring resonators is their high sensitivity to changes in the optical path length. This sensitivity can be exploited for various applications, such as sensors and optical switches. For instance, by monitoring the resonant wavelengths of a ring resonator, one can detect minute changes in the refractive index of the surrounding medium, which can be attributed to temperature variations, pressure changes, or the presence of analytes in a sensing scenario.Another important aspect of fiber optic ring resonators is their tunability. By incorporating materials with tunable refractive indices into the resonator, one canshift the resonant wavelengths dynamically. This tunability is crucial for dynamic control of optical systems and enables applications such as wavelength-routing in optical communication networks.In addition to their sensing and tunable properties,fiber optic ring resonators also find use in optical filtering and wavelength selection. The resonant nature of these resonators allows them to select specific wavelengths from a broadband optical signal, making them useful components in wavelength-division multiplexing (WDM) systems.The design and fabrication of fiber optic ring resonators involve precise control over the dimensions and refractive index of the waveguide. Modern techniques, such as femtosecond laser writing and precision fiber drawing, have enabled the creation of resonators with ultra-high finesse and narrow linewidths, enhancing their performance in various applications.In conclusion, fiber optic ring resonators have emerged as versatile and powerful components in optical systems. Their unique properties, including high sensitivity, tunability, and wavelength selectivity, make them invaluable for applications ranging from sensing andoptical switching to wavelength routing and filtering. As technology continues to advance, we can expect theseresonators to play an increasingly important role in the development of next-generation optical systems.。
北大老师张帆简历
张帆北京大学副教授,洪堡学者,2002年获北京邮电大学电磁场与微波技术专业工学博士学位。
2002年10月至2004 年11月任香港城市大学高级副研究员,2004年12月至2006年5月任柏林工业大学洪堡研究员。
2006年5月底加入北京大学任职副教授。
张帆博士现为美国电子电气工程师协会IEEE会员和美国光学学会OSA 会员。
由于在洪堡研究员期间出色的科研工作,德国洪堡基金会向他及北京大学赠送了价值近2万欧元的仪器设备-VPI光通信模拟软件。
张帆博士在区域光纤通信网与新型光通信系统国家重点实验室从事高速光纤通信系统、新型光调制格式、电均衡技术、相干光通信系统等方面的研究,并负责光纤通信国家重点实验室新型光传输实验平台的建设。
张帆博士在高速光纤传输、光脉冲非线性相互作用、相干光纤通信系统、电均衡、光学混沌通信等领域做出了多项创新性成果。
近年来在国内外重要学术期刊和会议上发表学术论文50余篇,其中包括国际会议邀请报告5篇。
论文被SCI数据库收录28篇,被SCI数据库论文引用50余次。
联系地址:区域光纤通信网及新型光纤通信系统国家重点实验室 2413房间北京大学信息科学技术学院,北京,100871Tel: 86-10-62761771(O)Email: fzhang@研究兴趣高速光纤通信系统;新型调制格式;相干光通信系统;数字信号处理与电均衡技术获奖∙2006 年德国洪堡基金会仪器设备资助-赠送VPI软件∙2004年德国洪堡基金会研究奖学金( Humboldt Research fellowships )∙2002 年北京邮电大学首届“学术新星”∙2000 年陕西省科技进步二等奖∙1998 年中国科学院科技进步二等奖∙1998 年中科院刘永龄奖学金科研经历∙“高速光通信系统和网络中传输损伤的研究”,德国洪堡基金项目,柏林工业大学。
∙“基于光纤中同步光学混沌的保密WDM通信系统”, 香港研究资助局项目,香港城市大学。
分光器稀疏配置约束下动态多播路由算法设计与仿真
密级分类号UDC学位论文分光器稀疏配置约束下动态多播路由算法设计与仿真者姓名:王晓静导教师:杜荔副教授东北大学信息科学与工程学院请学位级别:硕士学科类别:工学科专业名称:通信与信息系统文提交日期:2010年6月论文答辩日期:2010年6月位授予日期:答辩委员会主席:荡汐民阅人:茸逮竖、砉r磊尔北人学2010年6月AThesisinTeleommunicationsandInformationSystemsMulticastDesignandSimulationofDynamicRoutingAlgorithmwithSparseLightSplitterConfigurationConstraintbyWangXiaojingSupervisor:AssociateProfessorDuLiNortheasternUniversityJune2010)独创性声明本人声明,所呈交的学位论文是在导师的指导下完成的。
论文中取得的研究成果除加以标注和致谢的地方外,不包含其他人己经发表或撰写过的研究成果,也不包括本人为获得其他学位而使用过的材料。
与我一同工作的同志对本研究所做的任何贡献均己在论文中作了明确的说明并表示谢=艺思0学位论文作者签名:王眈穆日期:2汐,汐.6、瑚学位论文版权使用授权书本学位论文作者和指导教师完全了解东北大学有关保留、使用学位论文的规定:即学校有权保留并向国家有关部门或机构送交论文的复印件和磁盘,允许论文被查阅和借阅。
本人同意东北大学可以将学位论文的全部或部分内容编入有关数据库进行检索、交流。
作者和导师同意网上交流的时间为作者获得学位后:半年口一年口一年半口学位论文作者签名:王吼穆签字日期:2.010、6、28/’两年西导师签名:签字日期:杠荔ZOl口.‘、28东北大学硕士学位论文摘要分光器稀疏配置约束下动态多播路由算法设计与仿真摘要多播路由和波长分配是光网络多播研究的一个重要方面,与IP层多播相比,光层多播有一些特殊约束,包括波长连续性约束、分光节点稀疏配置约束、能量损伤约束。
光模块手册
6G S F P + T r a n s c e i v e r M T R S -6E 31-01DescriptionMTRS-6E31-01 is a high performance, cost effective modules, which is supporting Multi Rate 1.25-8.6Gbps, and transmission distance up to 10km on SM fiber. The transceiver consists of two sections: The transmitter section incorporates a 1310nm DFB driver and re-timer. The receiver section consists of a PIN photodiode integrated with a transimpedance preamplifier (TIA). The module is hot pluggable into the 20-pin connector. The high-speed electrical interface is base on low voltage logic, with nominal 100 Ohms differential impedance and AC coupled in the module.The optical output can be disabled by LVTTL logic high-level input of TX_DIS. Transmit Fault (Tx_Fault) is provided to indicate that the module transmitter has detected a fault condition related to laser operation or safety. Loss of signal (RX_LOS) output is provided to indicate the loss of an input optical signal of receiver. A serial EEPROM in the transceiver allows the user to access transceiver monitoring and configuration data via the 2-wire SFP Management Interface. This interface uses a single address, A0h, with a memory map divided into a lower and upper area. Basic digital diagnostic (DD) data is held in the lower area while specific data is held in a series of tables in the high memory area.Features● Up to 10KM transmission distance ● Support Multi Rate 1.25-8.6Gbps ●1310nm DFB and PIN receiver ●SFI electrical interface● 2-wire interface for integrated Digital Diagnostic monitoring ● SFP+ MSA package with duplex LC connector ● Hot pluggable ● Very low EMI and excellent ESD protection ● +3.3V power supply ● Power consumption less than 1W ● Operating case temperature: -40~+85°C Applications ● High-speed storage area networks ● Computer cluster cross-connect ● Custom high-speed data pipes ● LTE optical repeater application Compliance ● Compliant with Fiber Channel(FC)-Standard INCITS 352 ●Compliant with IEEE 802.3ae-2002● Compliant with FCC 47 CFR Part 15, Class B ● Compliant with FDA 21 CFR 1040.10 and 1040.11, Class I except for deviations pursuantSpecificationAbsolute Maximum RatingsUnit Storage Temperature T S-40 +85 ℃Supply Voltage V CC3 0 3.6 V Relative Humidity RH 5 +95 %RX Input Average Power Pmax - 3 dBmRecommended Operating ConditionsMax. Unit Operating Case Temperature T C-40 25 +85 ℃VV CC3 3.13 3.3 3.47Power Supply VoltageI CC3300 mAPower Dissipation P D 1 WData Rate 8.6 Gbps Transmission Distance 10 Km Transmitter Operating Characteristic-Optical, ElectricalUnit NoteSpectral Width(-20dB)Pm - - 1 nmSide Mode Suppression Ratio SMSR 35 - dBmLaser Off Power Poff - - -30 dBmExtinction Ratio ER 3.5 - - dBTransmitter Dispersion Penalty TDP - - 3.2 dBRelative Intensity Noise Rin - - -128 dB/HzOptical Return Loss Tolerance 12 - - dBOperating Data Rate 8.6 GbpsCentre Wavelength λC1260 1310 1355 nm Note1Average Optical Power Pavg -8.2 - 0.5 dBm Note1Optical Eye Mask Compliant with IEEE 802.3ae Note2Single Ended Output Voltage Tolerance -0.3 4 VCommon mode voltage tolerance 15 - mVTx Input Diff Voltage VI 180 700 mVTx Fault VoL -0.3 0.4 V At 0.7mAData Dependent Input Jitter DDJ 0.1 UIData Input Total Jitter TJ 0.28 UINotes:[1] Average optical power shall be measured using the methods specified in TIA/EIA-455-95.[2] Vertical eye closure penalty and stressed eye jitter are the test conditions for measuring stressed receiversensitivity. They are not the required characteristic of the receiver.Receiver Operating Characteristic-Optical, ElectricalUnit Note Center Wavelength λr 1260 1310 1360 nmReceiver Sensitivity (OMA) Psens -14.4 dBmStressed Sensitivity (OMA) -12.6 dBmLos Assert LosA -30 - dBmLos Dessert LosD -16 dBmLos Hysteresis LosH 0.5 - dBOverload Pin 0.5 dBmStressed Eye Jitter 0.3 UIp-p Note1 Receive electrical 3dB upper cutoff frequency12.3 GHzVertical Eye Closure Penalty 2.2 dB Note2 Receiver Reflectance -12 dBOperating Data Rate 8.6 GbpsSingle Ended Output Voltage Tolerance -0.3 4 VRx Output Diff Voltage Vo 450 850 mVRx Output Rise and Fall Time Tr/Tf 30 ps 20% to 80% Total Jitter TJ 0.7 UIDeterministic Jitter DJ 0.42 UINotes:[1] Receiver sensitivity is informative. Stressed receiver sensitivity shall be measured with conformance test signalfor BER =1x 10-12 .[2] Vertical eye closure penalty and stressed eye jitter are the test conditions for measuring stressed receiversensitivity. They are not the required characteristic of the receiver.Control and Status I/O Timing CharacteristicsNoteTX Disable Assert Time t_off 10 µs Note1TX Disable Negate Time t_on 1 ms Note2 Time to initialize including reset of TX_Fault t_init 300 ms Note3TX Fault Assert Time t_fault 100 µs Note4TX Disable to reset t_reset 10 µs Note5LOS Assert Time t_loss_on 100 µs Note6LOS Deassert Time t_loss_off 100 µs Note7Rate-Select Change Time t_ratesel 10 µs Note8 Serial ID Clock Rate f_serial_clock100 kHzNotes:[1] Time from rising edge of TX Disable to when the optical output falls below 10% of nominal[2] Time from falling edge of TX Disable to when the modulated optical output rises above 90% of nominal[3] From power on or negation of TX Fault using TX Disable[4] Time from fault to TX fault on[5] Time TX Disable must be held high to reset TX_fault[6] Time from LOS state to RX LOS assert[7] Time from non-LOS state to RX LOS deassert.[8] Time from rising or falling edge of Rate Select input until receiver bandwidth is in conformance with appropriatespecificationOptical Characteristics(Multi Rate Characteristics)4.95GTotal Power Consumption<1W <1W <1WTx Light Output Power >-8.2 >-8.2 >-8.2Extinction Ratio >3.5 >3.5 >3.5Eye Mask Margin >20% >20% >20%Rx Sensitivity <-22.0dBm <-20.0dBm <-17.0dBm-40~+85C -40~+85C -40~+85C WorkingTemperatureNotes:[1] For 1.25G data rate, the modules performance is compatible with 1G FC application but not fully compliant. If customer needs to fully compliant with 1.25G data rate specifications, we need to implement “Rate-Selection” function, please contact our sales team for detailed information.Pin-out DefinitionFigure1Pin AssignmentNote 1VeeT Module Transmitter Ground Note12 LVTTL-O TX_Fault Module Transmitter Fault Note23 LVTTL-I TX_Disable Transmitter Disable; Turns off transmitter laser output Note34 LVTTL-I/O SDA2-wire Serial Interface Data Line (Same as MOD-DEF2 as definedNote4in the INF-8074i)5 LVTTL-I/O SCL2-wire Serial Interface Clock (Same as MOD-DEF1 as defined inNote4the INF-8074i)6 MOD_ABS Module Absent, connected to VeeT or VeeR in the module Note57 LVTTL-I RS0Not used8 LVTTL-O RX_LOS Receiver Loss of Signal Indication (In FC designated as RX_LOS,in SONET designated as LOS, and in Ethernet designated at SignalNote2Detect)9 LVTTL-I RS1Not used10 VeeR Module Receiver Ground Note111 VeeR Module Receiver Ground Note112 CML-O RD-Receiver Inverted Data Output13 CML-O RD+Receiver Non-Inverted Data Output14 VeeR Module Receiver Ground Note115 VccR Module Receiver 3.3 V Supply16 VccT Module Transmitter 3.3 V Supply17 VeeT Module Transmitter Ground Note118 CML-I TD+Transmitter Non-Inverted Data Input19 CML-I TD-Transmitter Inverted Data Input20 VeeT Module Transmitter Ground Note1 Notes:[1] The module signal ground pins, VeeR and VeeT, shall be isolated from the module case.[2] This pin is an open collector/drain output pin and shall be pulled up with 4.7k-10kohms to Host_Vcc on the hostboard. Pull ups can be connected to multiple power supplies, however the host board design shall ensure that no module pin has voltage exceeding module VccT/R + 0.5 V.[3] This pin is an open collector/drain input pin and shall be pulled up with 4.7k-10kohms to VccT in the module.[4] See sff-8431 4.2 2-wire Electrical Specifications .[5] This pin shall be pulled up with 4.7k-10kohms to Host_Vcc on the host board.Block Diagram of TransceiverFigure2Transmitter SectionThe transmitter converts 6.25Gbit/s serial PECL or CML electrical data into serial optical data compliant with the6GBASE-LR standard. An open collector compatible Transmit Disable (Tx_Dis) is provided. A logic “1,” or no connection on this pin will disable the laser from transmitting. A logic “0” on this pin provides normal operation. The transmitter has an internal automatic power control loop (APC) to ensure constant optical power output across supply voltage and temperature variations. An open collector compatible Transmit Fault (Tx_Fault) is provided.TX_Fault is a module output contact that when high, indicates that the module transmitter has detected a fault condition related to laser operation or safety. The TX_Fault output contact is an open drain/collector and shall be pulled up to the Vcc_Host in the host with a resistor in the range 4.7-10 kΩ. TX_Disable is a module input contact. When TX_Disable is asserted high or left open, the SFP+ module transmitter output shall be turned off. This contact shall be pulled up to VccT with a 4.7 kΩ to 10 kΩ resistorReceiver SectionThe receiver converts 10Gbit/s serial optical data into serial PECL/CML electrical data. An open collector compatible Loss of Signal is provided. Rx_LOS when high indicates an optical signal level below that specified in the relevant standard. The Rx_LOS contact is an open drain/collector output and shall be pulled up to Vcc_Host in the host with a resistor in the range 4.7-10 kΩ, or with an active termination. Power supply filtering is recommended for both the transmitter and receiver. The Rx_LOS signal is intended as a preliminary indication to the system in which the SFP+ is installed that the received signal strength is below the specified range. Such an indication typically points to non-installed cables, broken cables, or a disabled, failing or a powered off transmitter at the far end of the cable.Recommended Interface CircuitFigure3DimensionsFigure4Table 1: Key Mechanical DimensionsDigital Diagnostic Memory MapEEPROM InformationName of Field Hex Description0 1 Identifer 03 SFP1 1 Ext. Identifier 04 SFP function is defined by serial ID only2 1 Connector 07 LC Connector 3-10 8 Transceiver 00 Transceiver Codes11 1 Encoding 06 64B/66B 12 1 BR, Nominal 3F 6250Mb/s 13 1 Rate Identifier 00 Unspecified14 1 Length (9um) km 0A Transceiver transmit distance,10km 15 1 Length (9um) 100m 64 Transceiver transmit distance,10km 16 1 Length (50um)10m 00 Transceiver transmit distance 17 1 Length (62.5um) 10m 00 Transceiver transmit distance18 1 Length (Copper) 00 Not compliant 19 1 Length (50um OM3) 00Not compliant20-35 16 Vendor name 48 47 20 47 45 4E 55 49 4E 45 20 20 20 20 20 20“HG GENUINE” Vendor Name(ASCII)36 1 Reserved 00 37-39 3 Vendor OUI 00 00 0040-55 16 Vendor PN 4D 54 52 53 2D 36 45 3331 2D 30 31 20 20 20 20“M T R S -6E 31-01”P a r t N o .(ASCII)56-59 4 Vendor rev 31 2E 30 20 “1.0” (ASCII) 60-61 2 Wavelength 05 1E Transceiver wavelength621Reserved0063 1 CC_BASE AD Check code for Base ID Fields64-65 2 Options 001A TX_DISABLE, TX_FAULT and Loss of Signal implemented.66 1 BR,MAX 00 Not Specified67 1 BR,MIN 00 NotSpecified 68-83 16 Vendor SN SN(Variable) Serial Number of transceiver(ASCII). 84-91 8 Date code DC(Variable) Manufactory Date Code.92 1 Diagnostic MonitoringType68Digital diagnostic monitoringimplemented, “externally calibrated”is implemented93 1 EnhancedOptions F0Optional Alarm/Warning flagsimplemented for all monitored quantities, Optional Soft TX_Disable control and monitoring implemented, Optional Soft TX_FAULT monitoring implemented, Optional Soft RX_LOS monitoring implemented94 1SFF_8472Compliance01Includes functionality described inRev9.3 SFF-847295 1 CC_EXT CS(Variable) Check sum for Extended ID Field.96-127 32 Vendor Specific Read only Depends on customer informationFilled by zero128-255 128 Reserved Read only Filled by zeroOrdering InformationReach Others MTRS-6E31-01SFP+6G1310nm DFB-8.2—0.5dBm PIN<-14.4dBm -40~85℃10km DDM/RoHSRelated Product InformationMTRS-1E21-01SFP+10G1310nm FP-8.2—0.5dBm PIN<-14.4dBm-40~85℃2km DDM/RoHS MTRS-02X13-G SFP+10G1310nm DFB-8.2—0.5dBm PIN<-14.4dBm0~70℃10km DDM/RoHS MTRS-1E31-01SFP+10G1310nm DFB-8.2—0.5dBm PIN<-14.4dBm-40~85℃10km DDM/RoHS MTRS-1E20-01SFP+10G1310nm FP-8.2—0.5dBm PIN<-14.4dBm0~70℃2km DDM/RoHS MTRS-6E21-01SFP+6G1310nm FP-8.2—0.5dBm PIN<-14.4dBm-40~85℃2km DDM/RoHS MTRS-6E20-01SFP+6G1310nm FP-8.2—0.5dBm PIN<-14.4dBm0~70℃2km DDM/RoHS MTRS-6E30-01SFP+6G1310nm DFB-8.2—0.5dBm PIN<-14.4dBm0~70℃10km DDM/RoHSWuhan Huagong Genuine Optics Technology Co., LtdAddress: Science & Technology Region of HUST, Donghu High-Tech ZoneWuhan, Hubei Province, 430223, China●Tel: +86-27-87180102●Fax: +86-27-87180220Email: market@Website: StatementHG Genuine possesses the authority for ultimate explanation of all information contained in this document, which is subject to change without prior notice. All the information was obtained in specific environments; and HG Genuine will not be responsible for verifying the products performance in customers’ operating environments, neither liable for the performance of users' products. All information contained is only for the users' reference and shall not be considered as warranted characteristics. HG Genuine will not be liable for damages arising directly or indirectly from any use of the information contained in this document.Publishing Date: 2010-01-08Copyright HG GenuineAll Right Reserved。
光电子材料导论第一章 信息处理技术和材料-全光波长转换 (2)演示教学
The most important use will be for avoidance of wavelength blocking in optical cross connects in WDM networks.
Increase the flexibility and the capacity of the network for a fixed set of wavelengths.
The XGM SOA wavelength converter is polarization independent.
Long SOA has superior dynamic performance
Long SOA only has 30 nm bandwidth, whereas it is 60 nm for short SOA.
Smaller bandwidth gives larger differential gain at the short wavelength side of the gain peak, a larger extinction ratio of the converted signal is expected for the long SOA
Incorporating saturable absorbers, injection locked Y-lasers; FWM in optical fiber.
XG saturation characteristic.
A cw signal at the desired output wavelength is modulated by the gain variation, so after the SOA it carries the same information as the intensity modulated input signal.
光学仪器测量方法:镜面间距检测系统说明书
8th International Conference on Manufacturing Science and Engineering (ICMSE 2018)Design Method of the Measuring System for the Mirror Surface Spacingof a compound lensPing Zhong1,a,Shaohui Pan1,b, Zhisong Li2,c and Xingyu Gao1,d1College of Science, Donghua University, Shanghai 201620, PR China2College of Information Science and Technology, Donghua University, Shanghai 201620, PR China a b*****************,c****************,d*****************Keywords:Optical fiber low coherence interference, lens mirror space, Signal-to-noise ratio, Band-pass filter, least square methodAbstract:Based on the principle of low coherent light interference of optical fiber, a new method for detecting the distance between the mirror surfaces of a compound lens is proposed. Firstly, a system based on the principle of low coherent light interference is designed. Secondly, the frequency calculation method of interference signal of measurement system is put forward, and the band-pass filter is designed for interference signal to improve the signal-to-noise ratios. Based on the characteristics of low coherence light interference signal, the least squares symmetric peak location algorithm is proposed, which realizes the precise locating of the peak of the interferometric signal. Besides, the experiment of measuring the distance between the compound lens is carried out and the measurement error is analyzed.IntroductionIn the manufacture of optical instruments, the center thickness machining precision and assembly precision of the lens have an important influence on the imaging quality of the optical system. Especially in high-performance precision optical systems such as aviation, aerospace and microscope systems, there are strict control requirements for the lens center thickness and the mirror spacing. So, how to get high precision measurement results is a challenging topic. At present, the method for measuring distance between the mirror surfaces of a compound lens is mainly divided into two types, the one is contact measurement and the other is non-contact measurement. The structure of contact measurement is relatively simple, but it has a large defect itself, such as easy to scratch the lens and destroy the lens. The frequent contact between the surfaces of the probe and lens can also make the worn lenses and affect the measurement accuracy. Non-contact measurement system is relatively complex, but it can perform nondestructive testing on the lens group. It is mainly to measure the relative position of the mirror surface by measuring the reflection signal of the lens surface. The methods mainly include image method [1], axial dispersion [2], differential confocal method [3], image calibration method [4, 5], etc. Low-coherence optical interferometry, as the main detection method of non-contact measurement for optical devices, is one of the hotspots today. In this paper, based on the principle of low-coherence light interference, a system for measuring the lens spacing of the compound lens is designed and the main factors affecting the detection accuracy are studied, and the effective method for signal filtering and waveform peak location is proposed.Measurement principle and system design of lens spacingLow-coherence light interferometry [6-12] is an interferometric technique using a broad-spectrum light source as a coherent light source. The coherence length is short and the interference peak can be generated only when the optical path of the measured light and the reference light is equal, so it has a good spatial positioning characteristic. By calculating the distance between the interference peaks at the apex of the front and rear mirror surfaces, the lens group spacing and the center thickness of the lens can be calculated. In this paper, the basic structure of Michelson interferometer is adopted, in which the light emitted the light source is passed through the optical fiber coupler to produce the measured light and the reference light respectively. On the one hand, the reflected signal come from the different surfaces of the sample has a different optical path. On the other hand, the referenceCopyright © 2018, the Authors. Published by Atlantis Press.This is an open access article under the CC BY-NC license (/licenses/by-nc/4.0/). 649optical path will change with the position of the reference mirror. Only the reflected signal from a specific location of the sample can be coherent with the reference light, where the location of the maximum intensity of coherent signal corresponds to the equal optical path position. The structure of the lens spacing measurement system is designed as shown in Fig.1.Fig.1. Lens group spacing detection system diagramThe light emitted from the wide-spectrum light source SLD (center wavelength 1310 nm, half-wave width 85 nm) is split by the fiber coupler and then enters the circulator 1 and the circulator 2, and forms measurement light and reference light, respectively. In order to facilitate the installation and debug the detection system, the visible light with the wavelength of 660nm and the measured light are mixed in the wavelength division multiplexer, and then, they are projected onto the front and back surfaces of the lens group by the collimator and reflected by the front and back surfaces of the lenses in the compound lens. Finally, the reflected light is shot into the ring through the collimator and the wavelength division multiplexer and recoupled into the optical fiber system from the port 3. In the same way, the reference light is reflected by a movable plane reflector. The returned reference light is ejected through port 3 of the ring and interferes with the measured light in the optical fiber coupler. The returned reference light is ejected through port 3 of the ring and interferes with the measured light in the optical fiber coupler. The path of the reference light can be changed by driving a plane reflector to move uniformly in a straight line. When the optical path of the measured light is equal to that of the reference light, that is, when the optical path difference is zero, the interference signal is strongest, at this time the maximum wave peak signal can be detected by the computer.Since the measuring beam contains many light rays reflected from the front and rear surfaces of multiple lenses, there will be multiple sets of maximum wave peaks in the process of moving plane reflector. According to the relative position of two zero light path difference, the measurement of lens spacing of compound lens can be completed. In the process of measurement, the information of the plane reflector is recorded in real time by a high resolution grating scale displacement sensor. In order to suppress the common-mode noise of the system and improve the signal-to-noise ratio of the system as much as possible, the system proposed in this paper uses a balanced detector for the photoelectric conversion of the interference signal. Then the data acquisition card is controlled by the computer, and the signal is processed by the computer. In order to further suppress the noise, a signal filter is designed.Signal filtering and waveform peak locationDesign of band-pass filterIn the detection system, the intensity of reflected light of the plane mirror is higher than the intensity of the tested lens. When the intensity ratio of the incident light passing through the reference light and detection light is 50:50, the interference signal is very weak. Fig.2(a) shows the waveform of the interference signals. In this case, the peaks of interference signals are difficult to extract. Through experiments, we can set the intensity ratio of the incident light passing through the reference light and detection light as 80: 20, and the output interference signals are very obvious as shown inFig.2(b).650Fig.2. The comparison of interference signal intensity.(a) the waveform of the interference signals while theintensity ratio is 50:50; (b) the waveform of the interference signals while the intensity ratio is 80:20It can be seen from Fig.2 (b) that, although the strong contrast interference signal can be obtained by setting the light intensity ratio between the reference light and detection light, the interference signal are often mixed with noise, which directly affects the location of peak signal. In this paper, a band-pass filter is designed to suppress the noise signal and improve the signal-to-noise ratio [13,14].The center wavelength of the designed filter can be calculated. Assuming that the moving speed of the plane mirror on a guide rail is mm/s during detection process and the center wavelength of the broadband light source is λ nm, then the center wavelength ( f ) of the filter can be calculated by the Eq.(1):=(2 ∕ )×10 . (1)For the system designed in this paper, v is 3.78mm/s , the wavelength rang of the broadband light source is 1290∼1330 nm, λ is 1310nm , thus the f =5.77×10 kHz and the frequency range of a band-pass filter is from 4.77kHz to 6.77kHz , and the center frequency can be selected as 5.77kHz .Method for locating the peak of interference signalIn this paper, the location of the peak of interference signal is the key to detection of lens spacing and can be determined by extracting the signal envelope. According` to the principle of low coherence interference, the wave peak of interference signal represents the interference generation between the reference light and detection light at zero optical paths. For measuring system, as long as the optical path difference between the two peaks of the interferometric signal from the lens group is obtained, the distance between the lenses of compound lens can be obtained. A simple method is to use the peak signal to determine the location of the zero optical path difference. However, because the adjacent extreme signals are so close to each other, the noise introduced in the detection process can easily cause location error which will lead to poor repeatability accuracy of the measurement system. The Gauss fitting algorithm has the advantage of locating peaks, but it requires that the interference signal has good symmetry. So it cannot meet the requirements of the system designed in this paper. In this paper, a symmetric peak location algorithm based on the least square method is proposed.First, the acquired interference signals are preprocess. Fig.3(a) shows the primary signals collected. The position of the mean value of the intensity is set to the abscissa axis. Fig.3(b) shows the sum of the absolute values for the same position signals. The envelope image of the signals is represented by a dotted line shown in Fig.3(b).According to the theory of partial coherence, when the value of function of the location points in envelope curve is greater than 1/e of the maximum value, these points are directly related to the coherence length of the light source. So the signals whose value is greater than 1/e of the maximum value point are selected as an effective processing signal, and then the location of peak signal can bedetermined by the a symmetric peak location algorithm based on least square. 651Fig.3. The method of locating signal peak.(a) The primary signals collected; (b) Envelope image of signal The method can be described as follows: i) Firstly, all points whose values are greater than 1/e of the maximum are selected, and then these points are plotted as a curve which called the original curve, it can be seen in Fig.4(a). After that, a symmetry axis which is parallel to the vertical axis and passes through the maximum value point of the original curve is drawn, then, the original curve revolves around the symmetry axis and forms another curve which is called revolved curve. ii) The revolved curve is moved left or right along the horizontal axis. Meanwhile, the mean square error between the original curve and the revolved curve is calculated. When the mean square error obtained is the smallest, the best translational position to the revolved curve is determined. iii) The revolved curve was moved according to the translation amount, as shown in Fig.4(b). Finally, the symmetrical position of the two curves is used as the zero-path difference position. The method utilizes the least squares method can equalize the errors brought by the interference signals and the measurement error and the system error can be effectively reduced.Fig.4. The method of locating wave crests.(a) Flip chart; (b) Flipping the curve after translationSpecular distance measurement experiment and error analysisAccording to the design principle of lens spacing detection system, a measurement system is set up as shown in Fig.5. Among them, the center wavelength of the detection system is 1310nm, and the half wavelength width of the SLD wide spectrum light source is 85nm, and its optical power is 10.8mW.Fig.5 Measurement test system for detecting the distance between the mirror surfaces of a compound lens (1) a wave division multiplexer, (2) Circulator 1, (3) 80/20 fiber couplers, (4) Circulator 2, (5) 50/50 opticalcouplers, (6) the single mode fiber , (7) balance detector652In order to test the measurement accuracy of the system designed in this article, an achromatic composite lens group is selected to perform experiment for detecting distance between the mirror surfaces. Among them, the compound lens includes 7 groups of lenses, and the structure of the combined lens is shown in Fig.6.Fig.6 The structure of the lens group to be measuredAccording to the experimental system and the detection algorithm, the measurement of the lens spacing of the compound lens is carried out. The interference signal improvement is very obvious, and the output interference signal waveform was shown in Fig.7(a), and Fig.7(b) is the waveform of the interference signal after filtered.Fig.7 Measurement of the waveforms of the interferometric signal in the lens group, (a) the waveforms of theinterfering signal before filtering,(b) the waveforms of the interfering signal after filteringIn order to evaluate the accuracy and stability of the test system, the lens group has been measured for many times. Table.1 lists the design values of the measured lenses, the average values of the ten measurements and the standard deviation calculated.Table.1 Measurement data of spacing thickness of lens groupSampleDesign thickness or spacing[mm] The mean value of measuring thickness or spacing [mm] Standard deviation[nm] Lens 15 .00 5.0327 59 Air gap 1-26.00 6.0155 101 Lens 25.00 4.9879 127 Air gap 2-35.00 5.0214 167 Lens 36.00 5.9897 201 Air gap 3-45.90 5.8591 221 Lens 46.00 6.0319 260 Air gap 4-58.00 7.9981 239 Lens 55.00 4.9794 327 Air gap 5-618.00 17.8951 389 Lens 65.00 5.0124 372 Air gap 6-77.00 6.9978 408 Lens 77.00 7.0214425 653According to the results of the measurement data, it can be seen that the relative intensity of the reflected light on the lens surface at the rear end of the lens group is weak and the standard deviation of measurement is relatively large due to the influence of the number of lenses contained a compound lens and the reflection loss of the lens surface. With the increase of the number of lens to be measured, the interference signal gradually get weakened and the precise of the positioning accuracy of the zero optical path difference position be reduced,which will lead to an increase in the measurement standard deviation in measuring the lens spacing of the compound lens.ConclusionIn this paper, based on the low coherent light interference method, a system for measuring the lens spacing of the compound lens is designed. A calculation method of interference signal frequency in measurement system is put forward, and a bandpass filter is designed, which can effectively improve the signal-to-noise ratio of the interferometric signal. The fitting method of the interference signal envelope is proposed. Based on the characteristics of the low-coherence interference signal, we used a least-squares correction information positioning method, which effectively improves the repeatability of the measurement. Finally, by testing the lens spacing of the combined lens, the effectiveness of the proposed design method is proved. The detection system not only is convenient, fast, and has no damage to optical devices, but also has high precision and strong stability. It has a good application prospect in optical processing and optical detection.AcknowledgementsThis work is supported by the National Natural Science Foundation of China (Grant No.51575099)References[1] A.V. Goncharov, L.L. Bailon and N.M. Devaney. Spie:Vol.7389(2009),p.738912.[2] M. Kunkel, J. Schulze. Glass Science and Technology: Vol.78(2005),p.245.[3] L.B. Shi, L.R. Qiu and Y. Wang. Chinese Journal of Scientific Instrument :Vol. 33(2012),p. 683.[4] H.W. Gao, H. Wang, Y.Y. Liu and Y. Yu. Journal of Electronic Measurement and Instrument:Vol.31(2017),p.820.[5] J.H. Zhang, Q Liu and R.H. Nie.Spie:Vol.36(2016),p.174.[6] P. Langehanenberg,A. Ruprecht. Spie:Vol.8844(2013),p.88444F.[7] J. Benitez, J. Mora.IEEE Photonics Technology Letters:Vol.29(2017),p.1735.[8] S. Merlo, P. Poma and E. Crisa. Sensors:Vol.17(2017).[9] O. Martinez-Matos, C. Rickenstorff and S. Zamora. Optics Express:Vol.25(2017),p.3222.[10] R. Abuter, M. Accardo and A .Amorim. Astronomy & Astrophysics:Vol.602(2017).[11] R.W Kunze, R. Schmitt. Tm-Technisches Messen:Vol.84(2017),p.575.[12] K.Li, M. Jiang, Z.Z. Zhao and Z.M.Wang. Optics Communications:Vol.389(2017),p.234.[13] J.M.Tang, H.W. Liu, Q.F. Zhang, B.P. Ren and Y.H. Liu. IEEE Transactions on AppliedSuperconductivity:Vol.28(2018).[14] H Lu, Z.Q. Yue and J.L. Zhao. Optics Communications:Vol.414(2018).654。
How to assign a wavelength channel in optical bus
专利名称:How to assign a wavelength channel in optical bus network发明人:オベルグ,マグナス申请号:JP1996524185申请日:19960202公开号:JP3677293B2公开日:20050727专利内容由知识产权出版社提供摘要: (57)< Abstract > The manner due to this invention N which is jointed mutually in series by the optical fiber of 1 pair has the node, it is simultaneous between all nodes of the bus network and it communicates the 2-way easily, it regards the channel allocation in the optical bus network. When suspension happens to the 1st pair fiber, the 2nd pair optical fiber which joints with the 1st node of the bus network and the 2nd node directly is adapted, although after the changing the conservation, containment aforementioned communication. Each of the transmitter of the bus network transmits the fixed network channel. Each of the receiver of the bus network receives the fixed wavelength channel, and makes that it passes through the other wavelength channel to the following node possible. The channel which is received by the receiver of one node is removed from the network completely, after that, it is possible to reuse this channel for transmitting the information between 2 other nodes. This way, it is possible to use the channel of minimum number for aforementioned communication between the nodes. In order for it to be possible, containment channel allocation when suspension happens in the optional dot of the bus network with the channel allocation modulo due to this invention, it is possible to allocate the channel of minimum number to the node of the optical bus network.申请人:テレフオンアクチーボラゲツト エル エム エリクソン(パブル)地址:スウェーデン国 エス-126 25 ストツクホルム(番地なし)国籍:SE代理人:浅村 皓,浅村 肇,清水 邦明,林 鉐三更多信息请下载全文后查看。
Optical wavelength conversion element and optical
专利名称:Optical wavelength conversion element and optical wavelength conversion module发明人:Sonoda, Shinichiro,Tsuruma, Isao,Hatori,Masami c/o Fuji Photo FilmCo.Ltd.,Matsumoto, Kenji c/o Fuji Photo FilmCo.Ltd.申请号:EP02022789.8申请日:19961206公开号:EP1302809B1公开日:20041006专利内容由知识产权出版社提供摘要:An optical wavelength conversion element (20) includes an optical waveguide (1) which is formed on a ferroelectric crystal substrate (2) having a nonlinear optical effect and extends along one surface (2a) of the substrate (2), and domain reversals (8) which are periodically formed in the optical waveguide (1) and arranged in a direction. The orientation of the spontaneous polarization of the substrate is reversed in the domain reversals and the optical wavelength conversion element converts the wavelength of a fundamental wave travelling in the direction in which the domain reversals are arranged under the guidance of the optical waveguide. The orientation of the spontaneous polarization of the substrate is at an angle θ larger than 0° and smaller than 90° to the surface of the substrate in a plane normal to the direction in which the fundamental wave is guided.申请人:FUJI PHOTO FILM CO LTD地址:JP国籍:JP代理机构:Klunker . Schmitt-Nilson . Hirsch 更多信息请下载全文后查看。
Dispersion measurement in optical networks
专利名称:Dispersion measurement in optical networks发明人:Mark Stephen Wight,Andreas Franz LudwigSizmann,Mei Du,Alan Glen Solheim申请号:US10058948申请日:20020128公开号:US20030142293A1公开日:20030731专利内容由知识产权出版社提供专利附图:摘要:A device for measuring dispersion of a link between two switching nodes of an optical network comprises a phase measuring unit PMU for determining a first phase of a data signal traveling on a first wavelength &lgr;1, and a second phase of the same datasignal traveling on a second wavelength &lgr;2, received consecutively over the link under measurement. A dispersion measurement controller controls operation of the phase measuring unit and characterizes the dispersion of the link at a wavelength of interest &lgr;=(&lgr;1+&lgr;2)/2, based on the first and second phases. The PMU includes a frame detector for determining a first and a second rotation signal indicative of the digital offset between the first and second test clocks with a respective frame start, and a phase detector for measuring the phase of these test clocks with respect to a static reference. The static reference is provided by the same data signal transmitted continuously over a reference wavelength. The test and reference clocks are 1:n divided to extend the range of the measurement. A method for characterizing the dispersion of a link of an optical network is also provided.申请人:INNOVANCE NETWORKS更多信息请下载全文后查看。
全光网波长转换器配置问题的一种启发式算法
全光网波长转换器配置问题的一种启发式算法吉玲;高随祥【期刊名称】《计算机仿真》【年(卷),期】2009(0)10【摘要】Wavelength conversion can eliminate the wavelength - continuity constraint and reduce the network blocking probability. Wavelength conversion is the key factor in minimizing the blocking probability and improving network performance in wavelength - routed all - optical networks. Spare wavelength converter placement is the key issue in all -optical networks. By analyzing every node with route amount through it, the route traffic , route length and centricity on routes, the paper proposes a heuristic wavelength converter allocation algorithms based on node's weight, and gives algorithms demonstration for general topology network .%波长转换技术可以消除全光网络中的波长一致性限制,降低网络阻塞率,因此在具有波长转换器的全光网中,如何通过合理配置、使用数量有限的波长转换器来最大程度的降低网络的阻塞率,这是全光网络需要解决的一个关键问题.因此对网络中通过节点的路由数量、通信量、路由长度及节点处于路由的中心距离进行分析,并给上述四个参数赋予一定的权重进行加权处理,提出了一种基于节点权的全光网络波长转换器配置算法,并针对一般拓扑网络进行了算法演示和分析.【总页数】4页(P138-141)【作者】吉玲;高随祥【作者单位】中国科学院研究生院,北京100039;中国科学院研究生院,北京100039【正文语种】中文【中图分类】TN929.11【相关文献】1.全光网络中波长转换器的优化配置算法 [J], 陈贞2.全光网络中波长转换器配置问题的蚁群算法 [J], 吉玲3.树形全光网络中波长转换器配置算法 [J], 刘志娟;高随祥;齐伟刚4.基于四波混频效应的波分复用全光网络波长转换器研究的新进展 [J],5.一种求解工程调度中多资源配置问题的启发式算法 [J], 王解法;李世敬;冯祖仁因版权原因,仅展示原文概要,查看原文内容请购买。
波长方程简述 Wavelength Equation Brief Explanation 英语
波长方程简述Wavelength Equation BriefExplanationBrief about Wavelength EquationThe distance between successive crests of a wave or higher points of electromagnetic waves is termed as wavelength. The frequency and wavelength are closely related to each other. But they are inversely proportionate to each other. The wavelength becomes shorter when the frequency is higher and the wavelength becomes longer when the frequency is lower. All the waves of light move with the same speed through a vacuum and the number of crest waves passing by a specific timeline depends onthe wavelengths. The wavelength is fundamentally denoted as Lambda which is a Greek Letter (λ). The wavelength formula or the wavelength equation of a wave has been represented as the following:(λ)=v/fHere, “v” represents the speed of the velocity of the Waves and “f” represents the frequency of the way. The wavelength is expressed in units of meters and the velocity is expressed in meters per second. The frequency is expressed in hertz. In a graph, we can see the waves which are graphed as functions of distance or time. The wavelength can be determined from the distance graph. On the other hand, frequency and period can be obtained from a time graph. Wave speed can be obtained from both the distance and timegraph. In calculating wavelength, the use of distance, speed, and time is found. Speed can be obtained by dividing the distance by time and speed can also be calculated by multiplying wavelength by frequency. Therefore, the wavelength can be calculated by dividing the distance by the product of frequency and time. Our Assignment Help Online expert will now give you the definition of wavelength.What is the wavelength?Wavelength in physics is considered to be the periodic wave’s special pe riod. The inverse or multiplicative inverse or reciprocal of the spatial frequency is the wavelength. In physics,mathematics, and engineering, special frequency is the feature of any structure which is periodic in space across the entire position. Special frequency can also be considered characteristic of a structure which is periodic through several positions in space. The spatial frequency measures the frequency of repeated movement of a structure’s sinusoidal components per unit of distance. Wavelength is generally determined by observing the distance between crests, zero crossing, and troughs which are the consecutive points of a similar phase. Wavelength is the characteristic feature of standing and travelling waves. It also depicts the patterns of the spatial wave. Greek letter Lambda (λ) is designated to wavelength. The term wavelength is applied in the domain of telecommunications and electronics where modulated waves are commonly found.Wavelength is also applied to the sinusoidal envelope of waves or modulated waves. The waves in the case of the sinusoidal envelope are developed by interferences of different sinusoids. In the domain of telecommunications and electronics, the process of varying single or multiple properties of a carrier signal is known as modulation. The carrier signal is the periodic waveform. The periodic waveform varies with modulating signal which typically provides information which is to be transmitted. If a sinusoidal wave is considered to be moving at particular wave speed, wave frequency is inversely proportional to wavelength. This means the waves which have higher frequencies would have shorter wavelengths.On the other hand, the waves which have lower frequencies will have much longer wavelengths.The medium such as vacuum, water, or air determines wavelength. The medium through which wave travels determines the wavelength. There are several wave-like phenomena such as light, sound waves, periodic electrical signals, and water waves. A sound wave is observed in air pressure as a variation. In light, the strength of the magnetic field and the electric varies. In electromagnetic radiation, the magnetic field and electric also vary. In the case of water waves, variations are found in the height of a water body. In the case of crystal lattice vibration, the atomic positions are found to vary. Therefore, wavelength measures the distance between the repetitions which we found in peaks, zero-crossing or valley-like shapes. It does not measure the distance a particular particle moves. The spectrum is the range of frequencies or wavelengths for wave. It is commonly usedconcerning the electromagnetic spectrum or vibration spectrum or sound spectrum. Therefore, a wavelength can be defined as the distance between successive points in an electromagnetic wave or sound wave.Repeated patterns which we observe in the case of travelling energy like light, sound, or light are represented by wavelengths. The distance between two similar or identical crests or peaks or high points is measured by a wavelength. The distance between two low points or troughs in a similar wave is also measured by wavelength. The wavelengths are distinctive in their formations and this formation plays a significant role in differentiating and energy from that of the other. Wavelengths are highly used in the field of technology and science. The engineers, scientists, technologies, use wavelengths toidentify different energy forms in the field of aerospace, network administration, and any other domain of technology. The wavelength of light it is found to vary with colours point the wavelength of light is different for each colour. For example, the longest wavelength is found in case of red colour and the least wavelength is found in the case of violet colour. The wavelength of infrared radiation is found to be longer even then the wavelength of red colour. Frequency and wavelength are inversely proportional to each other. It means the shorter the wavelength, higher is the frequency. On the other hand, longer the wavelength, lower will be the frequency. On an electromagnetic radiation spectrum, the wavelength is indicated by the distance between the repetitions which are observed in the waves. Radio waves which we find in audio range and waves are also includedin the electromagnetic radiation spectrum in a visible light range.How can wavelengths be measured?It is very important to understand the way a wavelength is measured. Wavelengths are generally measured with the help of the units of meters such as centimetres, millimetres, nanometres, meters, etc. Smaller denominations are also used such as picometres, nanometres, and centimetres in measuring shorter wavelengths. The smaller denominations of meters are usually used in measuring shorter wavelengths. The shorter wavelengths which we found find in the electromagnetic spectrum are measured by the help of smaller denominationsof meters. The wavelength such as x-rays, ultraviolet radiation, and gamma rays which are observed in the electromagnetic spectrum, are measured by the help of smaller denominations of meters such as picometres, nanometres, and centimetres. Optical spectrum analyzers or optical spectrometers are the instruments which are used in detecting wavelengths on an electromagnetic spectrum. The wavelength can be measured by the distance between two successive crests in the same wave. The wavelength is the distance between two crests or points in a wave. The distance between two peaks or valleys is the wavelength. in measuring wavelength, two important parameters are needed. these two parameters are frequency and wave speed. The frequency represents the number of cycles of wave passing point at a specified time. On the other hand, the speed ofthe waves is represented by the rate at which a wave can move through any medium and it is highly dependent on the propagation of the medium. For example, electromagnetic waves and sound waves travel through the air. The number of oscillations per unit of time in a wave is represented by the frequency of the wave. Shorter wavelengths can be observed if the frequency is higher and longer wavelengths are observed if the frequency is lower. This is because of the inverse relationship between the frequency of a wave and its wavelength. The wave speed can be calculated by multiplying the number of cycles which pass a point every second by the length of the cycle. The wave speed can be mathematically stated as the multiplication of cycle length and cycles per second. Now our experts from OnlineAssignment Help will tell you about the Wavelength Equation.Wavelength EquationThe characteristic patterns which we find in a light wave or radio wave or infrared wave have a particular length and shape. The distance between two consecutive peaks or high points in the same phase is known as a wavelength. The distance between two consecutive troughs or crests of a wave is the wavelength. Wavelength is measured in the wave’s direction. The distance from one trough or crest to the other and again from that trough or crest to another is the wavelength. The waves can be electromagnetic waves or a sound wave or evena light wave. The highest points where the trough of the wave is found to be the lowest is known as the crest. In measuring wavelength, units of lengths like centimetres, meters, nanometres, millimetres, etc. are used. Wavelength equation is also known as wavelength formula which depicts wavelength to be equal to the ratio between the speed of the waves and wave frequency. Therefore, it can be seen that a wavelength can be measured or calculated by dividing wave velocity by wave frequency. The wavelength is always represented meters. In the wavelength equation, “v” represents velocity and “f” represents frequency which is also measured in hertz or Hz.Wavelength equation is one of the well-known methods of calculating wavelength. The wavelength of any wave can be calculatedsimply by dividing the speed of the wave by its frequency. The wavelength equation or wavelength formula can be written as follows:Wavelength EquationWavelength =Velocity or speed of wave/FrequencyWavelength (λ) =Wave velocity or speed of wave (V)/frequency (f)λ = V/fIt is very important to use correct units in the wavelength equation so that the wavelength can be calculated accurately and the result can be expressed in a correct unit of measurement. Imperial and metric units can be used inrepresenting the speed of the wave. The units such as meter per second, kilometres per hour, and miles per hour, etc. can be used in representing speed. Wavelength is generally measured in metric units such as meters, nanometres, millimetres, etc. Frequency is always expressed in hertz which implies “per second”. The equation can be used in calculating wavelength with the help of certain data or information about the speed of the wave and its frequency. The known quantities can be plugged into the wavelength equation in calculating wavelength. If the wavelength of any wave is to be calculated then the frequency and speed of the wave need to be plugged into the equation. By dividing the speed of the wave by its frequency, the wavelength can be accurately calculated and obtained. Wavelength equation can help calculate wavelength depending on thegiven information about velocity and frequency. If information about frequency and speed of the wave is given, by using wavelength equation the wavelength can be easily calculated. In calculating the wavelength of light, information about specific photon energy needs to be obtained. With the help of the energy equation, the wavelength of light can be calculated. It is very important to use the current formula in calculating wavelength.For example, if a wave speed is 600m per/sec, and the wave frequency is 30waves/sec, the using wavelength equation we can calculate wavelength. The equation is the following:Wavelength=V/f (V=speed of the wave and f=wave frequency)Therefore, the wavelength is 20 mWavelength= 600/30=20mWavelength is the distance between two successive or consecutive crests or troughs of a similar wave. Things which can move are water, strings, air, ground-earthquake, and light. These things can move like a wave. Wavelength is the velocity or speed of a wave divided by the wave’s frequency. The wavelength equation or wavelength formula is represented as follows:Wavelength (λ) =Wa ve velocity or speed of wave (V)/frequency (f)λ = V/fThe velocity is the speed at which a wave moves in a particular direction and this velocity or the speed can be calculated by the units of meters per sec or m/sec or m/s. The frequency is the crests or troughs move through a particular point in a particular time and the formula of frequency is cycles/s or Hz. An example can be used to make wavelength equation simplified to get understood. If sound speed is almost 340m/s, the frequency of the wave is about 20.0cycles/sec, the wavelength can be calculated by using the wavelength equation in the following way:λ = V/fWavelength (λ) =Wave velocity or speed of wave (V) 340m/s / frequency (f) 20.0cycles/sWavelength (λ)= 17.0m In this way, the wavelength can be calculated.。
光波传输
A Cognitive Quality of Transmission Estimator forCore Optical NetworksTamara Jiménez,Juan Carlos Aguado,Ignacio de Miguel,Ramón J.Durán,Marianna Angelou,Member,IEEE, NoemíMerayo,Patricia Fernández,Rubén M.Lorenzo,Ioannis Tomkos,and Evaristo J.AbrilAbstract—We propose a cognitive Quality of Transmission (QoT)estimator for classifying lightpaths into high or low quality categories in impairment-aware wavelength-routed optical net-works.The technique is based on Case-Based Reasoning(CBR), an artificial intelligence technique which solves new problems by exploiting previous experiences,which are stored on a knowledge base.We also show that by including learning and forgetting techniques,the underlying knowledge base can be optimized, thus leading to a significant reduction on the computing time for on-line operation.The performance of the cognitive estimator is evaluated in a long haul and in an ultra-long haul network, and we demonstrate that it achieves more than98%successful classifications,and that it is up to four orders of magnitude faster when compared with a non-cognitive QoT estimator,the Q-Tool. Index Terms—Case-based reasoning(CBR),cognitive networks, impairment-aware networking,quality of transmission(QoT), wavelength-routed optical network(WRON).I.I NTRODUCTIONI N all-optical transparent networks,traffic is carried throughend-to-end wavelength channels,called lightpaths,without any type of Optical-Electrical-Optical conversion at interme-diate nodes.However,as optical signals traversefiber links and nodes,and propagate through active and passive optical com-ponents towards their destination,they suffer from a number of physical impairments which degrade the signal quality.These impairments affect each optical channel individually,but they also cause disturbance and interference between co-propagating channels.Hence,as there is no conversion to the electrical do-main and consequently,no regeneration at intermediate nodes, the Quality of Transmission(QoT)will be affected and might not comply with service requirements.Therefore,in the last years,the impact of physical layer impairments in optical net-work design and operation has received significant attention. As a result,this interest has led to a set of proposals that,forManuscript received October22,2012;revised December11,2012;accepted December28,2012.Date of current version January30,2013.This research has been supported by the CHRON(Cognitive Heterogeneous Reconfigurable Op-tical Network)project,with funding from the European Community’s Seventh Framework Programme[FP7/2007-2013]under grant agreement no.258644. The work of T.Jiménez was supported in part by the Council of Education of the Regional Government of Castilla-León and in part by the European Social Fund.T.Jiménez,J.C.Aguado,I.de Miguel,R.J.Durán,N.Merayo,P.Fernández, R.M.Lorenzo,E.J.Abril are with the University of Valladolid,47011Val-ladolid,Spain(e-mail:tamara.jimenez@tel.uva.es).M.Angelou and I.Tomkos are with the Athens Information Technology Center,19002Peania,Athens,Greece.Color versions of one or more of thefigures in this paper are available online at .Digital Object Identifier10.1109/JLT.2013.2240257instance,not only solve the Routing and Wavelength Assign-ment(RWA)problem in Wavelength-Routed Optical Networks (WRONs),but also ensure appropriate QoT on the established lightpaths[1],[2].For that aim,effective and efficient methods for predicting the QoT of lightpaths(before being established and measured)are required.In that way,such a predicting tool can be used to discard those lightpaths that will not fulfill QoT requirements,and also to verify that a new lightpath will not have a significant impact on existing ones,thus avoiding trou-blesome situations.In particular,Azodolmolky et al.[3],[4]have presented an impairment aware network planning and operation tool for all-optical and translucent networks.A key element of that tool is an integrated real-time quality of transmission estimator,the Q-Tool.This tool combines in a single framework a number of well investigated and verified analytical models previously pro-posed in the literature and,in contrast to other approaches,it also relies on a numerical split-step Fourier method in order to im-prove accuracy[3].The Q-Tool receives the topology(with its physical characteristics)and a set of lightpaths and then com-putes their associated Q-factors.The Q-factor is an indicator of the quality of transmission,which is related to the signal’s bit error rate(BER),so that a higher value of the Q-factor cor-responds to a lower BER[5].The Q-Tool provides relatively accurate estimates of the Q-factor by taking into account sev-eral models of linear and nonlinear impairments of the phys-ical layer,thus being a very useful element in optical network design and control.However,it suffers from a few limitations. First of all,it is only valid for10Gb/s OOK networks.Sec-ondly,due to the complex calculations required,the computing time is very high,ranging from1to1,000seconds,depending of the scenario,on the software implementation described in[6]. Therefore,the use of this tool may be prohibitive when time constraints are important for real time control;as well as for the application of a number of planning techniques,such as those based on genetic algorithms[7],since they rely on the evalua-tion of many alternative potential configurations.On the other hand,Poggiolini[8]has proposed a Gaussian Noise(GN)model which is able to estimate,quickly and ac-curately,the Optical Signal to Noise Ratio(OSNR)of the op-tical channels in uncompensated coherent transmission systems. Although this pioneering work opens the door for further de-velopments and enhancements,it does not yet address network scenarios(where channels coming from different locations are multiplexed in an opticalfiber at optical cross-connects),and it is not valid for dispersion compensated systems.In this paper,we propose an alternative approach for pre-dicting the quality of transmission of lightpaths in an optical0733-8724/$31.00©2013IEEEnetwork(i.e.,before being established),which consist on re-lying on cognition.Thus,by exploiting previous experiences (which are stored on a knowledge base),fast and correct de-cisions on whether a lightpath fulfills QoT requirements or not, can be made without having to rely on complex methods.In par-ticular,we propose a novel cognitive technique,based on Case-Based Reasoning(CBR)[9],which provides successful classi-fications of lightpaths into high or low QoT categories in more than98%cases,and that is several orders of magnitude faster than when using the Q-Tool;thus becoming a promising tech-nique for highly dynamic impairment-aware optical networks. The focus of this paper is set on the description of this novel technique,and on demonstrating the advantages of the use of cognition for QoT estimation.Since solid work on QoT esti-mation already exists for10Gb/s OOK networks,we have tar-geted the analysis of these scenarios in order to have a reliable baseline method for our comparisons.Considering this,we have selected the Q-Tool,as it gets a good balance between accu-racy(considering most of the physical impairments)and speed, thereby being a very good option to showcase the advantages and potential of the cognitive estimator.On the other hand,the fundamentals of the cognitive technique are generic enough to be applied to networks with higher data rates and,for instance, we have recently demonstrated its application in a WDM80 Gb/s PDM-QPSK system test bed[10].Therefore,it should be noted that the application of cognition to quality of transmis-sion assessment is the novel contribution of this paper,being the Q-Tool just used as a benchmark method for evaluating the capabilities of the cognitive mechanism under conditions as re-alistic as possible.The remaining of this paper is organized as follows.First of all,in Section II,we explain the fundamentals of the cogni-tive QoT estimator,which was introduced in[11],and discuss how the underlying knowledge base can be optimized by means of learning and forgetting techniques[12].Then in Section III, the performance of the cognitive QoT estimator is analyzed by means of a simulation study on a long-haul and in an ultra-long haul network,with different numbers of nodes,in order to analyze potential scalability issues.Moreover,we also discuss how the initial knowledge base can be built in pragmatic net-working scenarios.Finally,in Section IV,the main conclusions are stated.II.D ESCRIPTION OF THE C OGNITIVE Q O T E STIMATOR We have developed a cognitive QoT estimator which clas-sifies lightpaths into two categories:high and low QoT.These categories are determined by means of a user-defined threshold on the Q-factor.Thus,if the Q-factor of a light-path is higher or equal to this threshold,then it belongs to the high QoT category,and we assume that the lightpath complies with quality requirements.Otherwise,the lightpath belongs to the low QoT class.Alternatively,the classification can be done according to other QoT parameters like Error Vector Magnitude (EVM)values[5],[10],in this case being the values lower than the threshold those associated to the high QoT class.Neverthe-less,in this paper we focus on the Q-factor as the parameter determining the category of eachlightpath.Fig.1.Q-factor of the lightpaths,as a function of their lengths,in a simulation of the GÉANT2network for different network loads and32wavelengths per link.The cognitive estimator determines the QoT category of a lightpath by means of a hybrid mechanism.First,it takes into account the length of the lightpath,and then employs,if neces-sary,a Case-Based Reasoning system.The motivation for using the length as afirst element to classify the lightpath is its signif-icant impact on the Q-factor.As an example,Fig.1shows the Q-factor of different lightpaths depending on their total length.Thefigure has been obtained when simulating the GÉANT2network[13]as a dynamic WRON,equipped with32wavelengths per link and 10Gb/s OOK transceivers,for different network loads,and using the MATLAB implementation of the Q-Tool to evaluate the Q-factor of the lightpaths.The threshold to distinguish between high and low QoT categories has been set to16.9 dB(which corresponds to a BER of).As it can be observed,lightpaths shorter than a certain length(1,250km) generally belong to the high QoT category,while those with very long lengths(4,100km)typically belong to the low QoT class.However,there is an uncertainty area(i.e.,a range of intermediate lengths)where the rest of the characteristics of the lightpath also play an important role on its Q-factor and hence on its classification into a QoT category.Therefore,for classifying the lightpaths in this uncertainty area,a CBR system is applied.A.Case-Based Reasoning for QoT AssessmentCBR is a problem solving paradigm that emphasizes the role of prior experiences or cases stored in a Knowledge Base(KB) [9].In CBR,a new problem is solved:•by retrieving from the KB the most similar cases faced in the past to the problem currently tackled,•by reusing the retrieved cases,either directly or adapting them in order to provide a solution for the new problem,•by revising the proposed solution,i.e.,by checking its per-formance,•and by(maybe)retaining in the KB the new case and the solution employed.These steps can be implemented in different ways depending on thefinal application and the limiting factors like the max-imum time to provide the solution or the desired precision of the solution.An excellent review of the main techniques existing to implement a CBR system can be found in[14]. Particularly,in the CBR system of the cognitive QoT esti-mator,the initial KB is composed by a number of cases,which consist of a description of the lightpath(i.e.,a set of attributes) and its associated Q-factor.The description of the lightpath con-tains its route,that is,the set of links that it traverses(repre-sented by the percentage of their individual contribution to the total length of the lightpath),the selected wavelength,its total length,the sum of the co-propagating lightpaths per link,and the standard deviation of the number of total co-propagating light-paths.Moreover,the associated Q-factor stored in the KB is an estimate of the quality of transmission which has been obtained by using the Q-Tool.In order to obtain these cases,previous off-line simulations are executed.Therefore,the cases in the KB are different lightpaths established at different moments of those simulations,and their associated Q-factors are calculated off-line by means of the Q-Tool.The reason for selecting the Q-Tool along this study is that, as explained in the introduction,it combines several verified physical layer impairment models and numerical computations in order to provide more accurate values than other proposals. Nevertheless,it is important to note,that although we have used the Q-Tool for populating the KB,any other QoT estimator could be used instead and,in fact,it could be populated with data obtained from an optical communications system simu-lator or even coming from optical network monitors[15].(In Section III-B we will provide additional insights about these al-ternative procedures for building the KB.)In real network operation,where fast assessment of light-path quality is required,the cognitive QoT estimator works as follows.First,when facing a new lightpath request,the RWA problem is solved and the total length of the lightpath is cal-culated.If the length is lower than the lower threshold of the uncertainty area,the lightpath is assumed to fulfill the QoT re-quirements.On the other hand,if the length is higher than the upper threshold of the uncertainty area,it is assumed that the QoT requirements are not fulfilled.However,if the length be-longs to the uncertainty area,the CBR system is applied and it retrieves the most similar lightpath from the KB to the new request.In order to assess the similarity when comparing the new lightpath with each one contained in the KB,the at-tributes are normalized and the weighted Euclidean distance is calculated[16],[17]following(1),(1) where represents each attribute of the lightpaths and,is the weight associated to that attribute,and is the set of at-tributes.Thus,higher values(i.e.,closer to zero values)of(1) mean higher similarity of the cases.The set of weights used are the least-squares regression coefficients of a linear model for the KB considering the Q-factor as the dependent variable.The Q-factor of the new lightpath is assumed to be the same one than that of the retrieved case(i.e.,the most similar lightpath in the KB),and that value is used to decide whether the light-path fulfills the QoT requirements or not by comparing with the threshold value.In thisfirst version of the cognitive QoT estimator,the KB is completely static,and so it is not updated with new cases nor optimized,(i.e.,the retain stage of CBR is not used).This first version of the cognitive QoT estimator will be denoted as R-CBR(Regular-CBR).B.Optimization of the KBAs it was previously mentioned,the KB of a CBR system can be updated to include new experiences by storing the descrip-tion and solutions of new problems faced by the CBR system, i.e.,the CBR system can learn.Learning tends to increase the effectiveness of the system,as the KB grows.However,exces-sive learning has a great impact on retrieval time,which is in-cremented,as it strongly depends on the size of the KB[14]. This is known as the utility problem[14],[18]:the cost of main-taining and searching in a large case base outweighs the benefit of storing its knowledge.Therefore,to avoid the utility problem,not only learning but also forgetting techniques have to be implemented.Thus,case addition and deletion strategies should be implemented to con-trol retention and to eliminate cases that do not improve the per-formance of the system.Hence,in this subsection,we propose a mechanism to enhance the cognitive QoT estimator with the execution of periodic maintenance stages where the KB is up-dated and optimized.During the operation of the cognitive estimator,all cases whose classifications have been done by the CBR stage(i.e., lightpaths with lengths belonging to the uncertainty area) follow a double check.It is checked(1)if the new lightpath has been correctly classified in its QoT category,and(2),if the error between the Q-factor estimate obtained by the CBR system and its real value is below a certain amount(the permitted error, ).If(1)or(2)are not fulfilled,then the case is stored in an auxiliary database as a candidate to be incorporated to the KB(i.e.,to be learned).When the CBR system has made a certain number of classi-fications(either correct or wrong),the maintenance phase is ex-ecuted.It consists in,first,adding to the KB the cases stored as candidates to be learned(and then resetting the auxiliary data-base),and second,applying a technique to remove redundant cases from the KB.Specifically,the technique selected to carry out the redun-dancy removal is based on the Conservative Redundancy Re-duction(CRR)method[19].This algorithm aims at removing redundant cases which are not located near the class borders. To do this,the coverage set(CS)of each case is calculated.The coverage set of a case is the set of all cases that can success-fully classify[19],[20].Therefore,cases which have a large CS are probably situated in clusters of cases with the same classifi-cation.On the other hand,if a case has a small CS,this indicates that it has few neighbors,and therefore,it is situated close to a border of the class[19].The pseudo code to calculate the CS of each of the cases in the KB,adapted to the cognitive QoT esti-mator features,is shown in Table I.TABLE IP SEUDOCODE TO C ALCULATE THE C OVERAGE S ET OF A LL C ASES IN THEKB Once the CS has been calculated,the CRR algorithm sorts all cases in the KB in ascending order according to the size of their coverage set.Then,the cases in the KB are analyzed starting from that with the smallest CS,and the cases in its coverage set are removed from the KB [19].(Obviously,if a case is removed during this process,it will not be analyzed later to delete its own coverage set.)If after running these processes the size of the KB is higher than that of the original KB (i.e.,the KB that was generated before starting the whole optimization process),then an appro-priate number of cases is deleted from the KB,starting with those cases having a higher coverage set.Therefore,the resul-tant size of the KB is never higher than its initial size.Finally,it should be noticed that in order to apply the opti-mization procedure that we have just described,it is necessary to compare the estimated Q-factor for each lightpath with the real one.Hence,for real-time updates of the KB,the cognitive QoT estimator must work in collaboration with a network monitoring system (which measures the Q-factors of the established light-paths)and supported by appropriate network protocols.Nev-ertheless,in this paper,we focus on the off-line optimization of the KB.Hence,once an initial KB is generated by means of off-line simulations (as described in Section II-A),it is opti-mized by applying the procedure mentioned above.This is also done by means of an off-line simulation (i.e.,executed prior to online operation)which uses the Q-Tool to provide the “real”Q-factors.Summing up,we have proposed two different methods.The first one,referred as R-CBR (Regular CBR),is a cognitive QoT estimator that does not optimize the KB prior to online oper-ation (i.e.,it operates as described in Section II-A)[11].The second one,called FixE-CBR (Fixed Error CBR),is a cognitive estimator which applies learning and forgetting techniques in order to perform an off-line optimization of the KB with a fixedpermitted error[12].However,the KB associated to the FixE-CBR method is no further optimized during online operation.III.S IMULATION S CENARIOS AND R ESULTSA.Performance Evaluation of the Cognitive QoT Estimator To evaluate the performance of the two versions of the cogni-tive QoT estimator,simulations have been carried out in two dif-ferentnetworks in order to analyze potential scalability issues:TABLE IIL OW AND H IGH L ENGTH L IMIT OF THE U NCERTAINTY A REAa long haul network,the 14-node Deutsche Telekom (DT)net-work [3],and an ultra-long haul network,the 34-node GÉANT2network [13].Both networks have been con figured as dynamic WRONs and equipped with 10Gb/s OOK transceivers.Each link consists of a number of spans formed by Standard Single Mode Fiber (SMF)and Dispersion Compensating Fiber (DCF),and 32and 64wavelengths per link have been considered.The results have been obtained by analyzing the networking sce-narios under different traf fic loads,and the traf fic loads for the DT and GÉANT2networks have been selected so that they lead to a similar range of blocking probabilities.For the DT network,traf fic loads from 0.3to 2.0for the 32wavelengths scenario,and from 0.5to 4.1for the 64wavelengths scenario,have been considered.For the GÉANT2network,the considered network loads have been 0.1to 0.45,and 0.1to 1.0,for the 32and 64wavelengths scenarios,respectively.A traf fic load of 1means that,in average,if there were no blocking,there would be one lightpath established between each source-destination pair in the network.The routes and wavelengths for the connections have been obtained by means of an adaptive RWA algorithm (AUR-Exhaustive)[21],since it offers more flexibility and thus a much lower blocking probability in dynamic scenarios than other approaches based on the utilization of fixed pre-calculated routes [21],[22].Two implementations of the Q-Tool were developed in the framework of the European Union DICONET project [3],[4]:a MATLAB implementation,and a hardware implementation (based on an FPGA)which accelerates the QoT estimation process [6].With the aim of providing a fair comparison in terms of computing time,the cognitive QoT estimator has also been implemented in MATLAB,and thus it will be compared with the software implementation of the Q-Tool.The Q-factor threshold for the classi fication of lightpaths into high or low QoT categories has been set to 16.9dB (i.e.,distinguishing between BER lower and higher than ,respectively).Moreover,by means of simulation,the limits (in terms of lightpath length)of the uncertainty area have been determined so that the probability of successful classi fication is higher than 99.99%outside the uncertainty area.The limit lengths for both networks can be found in Table II.The initial KB of the CBR system has been populated with different numbers of cases,running from 500to 5,000for the DT network and from 5,000to 50,000for GÉANT2.In order to ensure a fair comparison between both networks,the size of the KBs involved in the GÉANT2network has been increased,since it has a higher number of nodes involved (the number of source-destination pairs increases by 6times from the DT to the GÉANT2network).The cases of the KB for both networks have been chosen randomly from those generated in an off-line sim-ulation.Each KB provides coverage of the uncertainty area forFig. 2.Successful classifications of QoT when comparing R-CBR and FixE-CBR methods for DT network.The numbers that appear next to the FixE-CBR points refer to the initial sizes of the KB before executing the optimization procedure.all traffic loads,so that the same KB can be used independently of the traffic load faced by the network.When operating with an optimized KB(i.e.,for FixE-CBR), an off-line KB optimization process has been executed.For that objective,6,000new lightpaths for DT and36,000for GÉANT2,belonging to the uncertainty area,have been classi-fied,running the optimization process described in Section II-B after every500classifications.The permitted errorwhen optimizing the KB has been set to3dB.Once the optimization process hasfinished,the performance of the cognitive QoT estimator is analyzed.For that aim,other 6,000lightpaths in the DT network and36,000in GÉANT2net-work(belonging to both the certainty and uncertainty areas) have been evaluated.However,the KB is no longer updated during this evaluation,i.e.,there is no additional learning during the evaluation.The results that we show in the followingfigures have been obtained after repeating this process100times with different KBs.Average results are represented together with95%con-fidence intervals(although in most cases the size of the confi-dence intervals is smaller than the size of the symbols).Fig.2represents the percentage of successful classifications of lightpaths into high or low QoT categories for the DT network when employing the R-CBR and FixE-CBR estimators,that is, it compares the successful classifications when the KB has not been optimized before online operation,and when it has been optimized with afixed error policy.In thefigure,the numbers written next to the points associated to the FixE-CBR method indicate the size of the initial KB(i.e.,before being optimized). As shown in thefigure,even when the KB is not optimized (R-CBR),the percentage of successful classifications is very high.For the smallest size of the KB(500cases),the cognitive QoT estimator achieves more than99.45%correct classifica-tions,and that percentage raises to99.8%for the highest size of the KB considered in the simulation(5,000cases).When R-CBR and FixE-CBR are compared,not only is the percentage of successful classifications with an optimizedKB Fig. 3.Successful classifications of QoT when comparing R-CBR and FixE-CBR methods for GÉANT2network.The numbers that appear next to the FixE-CBR points refer to the initial sizes of the KB before executing the optimization procedure.(FixE-CBR)higher than without optimization(R-CBR),but also the number of cases in thefinal KB is typically much lower with FixE-CBR.For example,for32wavelengths,and a KB with an initial size of500cases and afinal size of412 cases,the percentage of successful classifications raises from 99.53%to99.84%.On the other hand,for an initial size of the KB equal to5000cases,and again for the32wavelengths scenario,FixE-CBR slightly raises the percentage of successful classifications from99.84%(R-CBR)to99.89%and,more importantly,it achieves a significant reduction of the size of the KB,as thefinal KB only contains618cases versus the5,000 initial cases(i.e.,87.64%reduction).As we will demonstrate later,this fact has a significant impact in terms of reducing the computing time.For the GÉANT2network,a similar behavior can be ob-served.Fig.3compares the evolution of the percentage of suc-cessful classifications when the KB size is increased for R-CBR and FixE-CBR for this network.As it can be seen,for the32 wavelengths scenario,the highest percentage of successful clas-sifications reaches98%for a KB of50,000cases,and99.15% when considering64wavelengths and the same size of the KB. Moreover,FixE-CBR improves the percentage of successful classifications for small KB sizes.For example,for64wave-lengths and an initial KB size of5,000cases,the percentage raises from95.4%to97%.However,again,the greatest impact of FixE-CBR is the significant reduction in the size of the KB. In this way,for64wavelengths,Fix-CBR reduces the KB size from50000to9404cases(i.e.,81.19%reduction).These results seem to indicate that there is a scalability problem,as the results for the GÉANT2network are slightly worse than for the DT.Therefore,we have analyzed this issue in more detail.The cognitive estimator relies on a hybrid mechanism thatfirst decides by means of a threshold length,and then, if required,by a CBR system.As previously described,the threshold lengths have been set so that when a classification。
基于PCE的WSON光网络RWA分配策略与仿真
基于PCE的WSON光网络RWA分配策略与仿真柳刚【期刊名称】《光通信技术》【年(卷),期】2012(36)11【摘要】为了有效分配WSON光网络中的波长资源,提出了一种基于路径计算单元(Path Computation Element,PCE)的波长交换光网络(Wavelength-Switched Optical Network,WSON)路由与波长分配策略.该策略通过PCE建立波长资源冲突避免表,并由目的节点与PCE进行通信确认,避免资源竞争问题的发生.将该策略下的网络阻塞情况与FF算法、RF算法进行对比仿真,仿真结果表明运用该策略可以有效抑制波长预留冲突,大大降低网络阻塞率.%In order to effectively assign wavelength resource in WSON optical network, a routing and wavelength assignment strategy in WSON optical network based on PCE is put forward. The strategy establishes wavelength resource collision avoidance table by PCE, and destination nodes communicate with PCE to notarize the table, which can avoid the occurrence of resource competition problem. Finally, the network blocking probability of the strategy is contrasted with FF algorithm and RF algorithm by simulation. The results of simulation demonstrate that utilizing the strategy can effectively restrain the wavelength reservation collision, and greatly reduce the network blocking probability.【总页数】3页(P22-24)【作者】柳刚【作者单位】西昌学院,四川西昌615013【正文语种】中文【中图分类】TN915【相关文献】1.基于分层图模型的静态RWA算法的仿真实现 [J], 赵蕾;路振山;李峥2.WDM光网络中动态RWA算法仿真的实现 [J], 郑亚彬;王荣;项鹏3.基于网络编码的光组播树优化RWA研究 [J], 周迎富;阳小龙4.基于遗传算法的大规模WDM光网络RWA算法 [J], 张敏;许渤;蔡怡;武保剑;邱昆5.波长路由光网络中RWA算法的仿真系统设计 [J], 张曙光;李正贤因版权原因,仅展示原文概要,查看原文内容请购买。
【光纤中的色散效应】dispersion phenomena in optical fibers
dispersion
3. Dispersion types
Dispersion represents a broad class of phenomena related to the fact that the velocity of the electromagnetic wave depends on the wavelength. In telecommunication the term of dispersion is used to describe the processes which cause that the signal carried by the electromagnetic wave and propagating in an optical fiber is degradated as a result of the dispersion phenomena. This degradation occurs because the different components of radiation having different frequencies propagate with different velocities. We distinguish various kinds of dispersion and all of them will be discussed in this chapter:
Fig.3.1. Attenuation caused by dispersion at transmission speed a) 0.78 Gb/s, b) 1.33 Gb/s, c) 3.11 Gb/s for the optical fiber characterized by the chromatic dispersion of 17 ps/nm/km and propagating the light from the single-mode laser DFB at spectral width of 0.1 nm Usually, the maximum attenuation caused by dispersion can be tolerated up to the value of 2 dB, which means that at the transmission speed of 3.11 Gb/s we might apply the optical fiber with length up to 85 km without any regeneration. We can see that for the transmission speeds higher than 3 Gb/s dispersion plays an key role in case of larger distances and the transmission becomes dispersion-limited. Simply speaking, chromatic dispersion means that the different wavelengths travel with different velocities even for the single-mode optical fibers. The chromatic dispersion is the characteristic feature of the material and it is imposible to avoid it, it can be only reduced. The dependence of the refraction index on the wavelegth for fused silica is shown in the Figure 3.2.
光电子材料导论第一章 信息处理技术和材料-全光波长转换
World's first widely-tunable all-optical wavelength converter, designed and fabricated at UCSB
2
The most important use will be for avoidance of wavelength blocking in optical cross connects in WDM networks.
20
四波混频全光波长转换
21
Energy-level diagram for dualwavelength-pumped Ramanresonant FWM process. Conversion of the weak primary pump wave P1 to the corresponding first Stokes wave S1(P1) is achieved by strong phonon prepared by the intense secondary pump wave P2 and the corresponding first Stokes wave S1(P2).
All-optical wavelength conversion
To “imprint” digital information from one wavelength of to another wavelength without passing the signal through electronics Critical next step in the evolution of optical networks and photonic packet switching.
光电子材料导论第一章 信息处理技术和材料-全光波长转换 (2)-PPT文档资料22页
All-optical wavelength converters:
Semiconductor optical amplifiers(SOA) in cross gain modulation (XGM)
Cross phase modulation (XPM), Four wave mixing (FWM), bistable lasers
• Large wavelength span for both input and output signals.
• Possibility for same input and output wavelengths (no conversion).
• Low chirp • Fast setup time of output wavelength • Insensitivity to input signal polarization • Simple implementation
The XGM SOA wavelength converter isБайду номын сангаасpolarization independent.
Long SOA has superior dynamic performance
Long SOA only has 30 nm bandwidth, whereas it is 60 nm for short SOA.
Wavelength conversion technologies
Electro-optic converter consisting of a detector followed by a laser that retransmits the incoming signal on the new wavelength. Complexity Large power consumption Speed limitation
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Wavelength Assignment in Optical Networkswith Fixed Fiber CapacityMatthew Andrews and Lisa ZhangBell Laboratories,600Mountain Avenue,Murray Hill,NJ07974{andrews,ylz}@Abstract.We consider the problem of assigning wavelengths to de-mands in an optical network of m links.We assume that the route ofeach demand isfixed and the number of wavelengths available on afiberis some parameterµ.Our aim is to minimize the maximum ratio be-tween the number offibers deployed on a link e and the number offibersrequired on the same link e when wavelength assignment is allowed tobe fractional.Our main results are negative ones.We show that there is no constant-factor approximation algorithm unless NP⊆ZPP.No such negative re-sult is known if the routes are notfixed.In addition,unless all lan-guages in NP have randomized algorithms with expected running timeO(n polylog(n)),we show that there is no logγµapproximation for anyγ∈(0,1)and no logγm approximation for anyγ∈(0,0.5).Our anal-ysis is based on hardness results for the problem of approximating thechromatic number in a graph.On the positive side,we present algorithms with approximation ratiosO(log m+logµ),O(log D max+logµ)and O(D max)respectively.HereD max is the length of the longest path.We conclude by presenting two variants of the problem and discussingwhich of our results still apply.Keywords:Optical networking,wavelength assignment,fixed capacityfiber, inapproximability.1IntroductionWe consider the problem of achieving transparency in optical networks.A path is said to be routed transparently if it is assigned the same wavelength from its source to its destination.Transparency is desirable since wavelength conversion is expensive and defeats the advantage of all optical transmission.More formally,we consider an optical network consisting of vertices and optical links and a set of demands each of which needs to be routed from a source vertex to a destination vertex on a single wavelength.Each optical link has one or multiple parallelfibers deployed.The fundamental constraint is that for each wavelengthλ,eachfiber can carry at most one demand that is assigned wavelengthλ.A common problem is to minimize the number of wavelengthsrequired so that all demands can be routed assuming onefiber per link.However, in reality a more pertinent problem is that the number of wavelengths that each fiber can carry isfixed to some valueµ,i.e.the total number of wavelengths is fixed.(For example,[11]lists thefiber capacities from different vendors.)The problem now is to minimize the number offibers required.For most service providers,the cost of afiber on a link can be divided into two components.First,there is the cost of renting thefiber from a“dark-fiber”provider.Second,there is the cost of purchasing optical equipment to“light”the fiber.When networks are being designed,the exact form of these costs are of-ten not well known.For example,the dark-fiber providers may regularly update their rental rates and the cost of optical equipment may be subject to negotia-tion.Moreover,the service providers may have to rent from different dark-fiber providers in different parts of the country and each may have different pricing strategies.Therefore,over time thefiber cost may vary nonuniformly from link to link.Despite this,we do know that the number offibers we use on a link must be at least the total number of demands routed through the link divided by the number of wavelengths perfiber.One robust way to ensure our network cost is low regardless of the exact cost structure is to minimize the ratio between the number offibers actually used on the link and this lower bound.In this paper we assume that the path followed by each demand is already fixed.Wavelength assignment is therefore the only problem.In an alternative formulation,routing and wavelength assignment could be performed simultane-ously.However,in many practical situations arising in optical network design, routing is determined by some higher-level specifications(e.g.carriers may re-quire min-hop routing,see[10]).Hence,it is important to consider the wave-length assignment problem in isolation.We also remark that once a demand is assigned a wavelength,whichfiber on each link actually carries the demand is not an issue.This is because modern optical devices such as mesh optical add-drop multiplexers allow distinct wavelengths from differentfibers to be multiplexed into a newfiber.Fiber minimization withfixed routing is NP-hard on networks with general topology(by a simple reduction from graph coloring).In this paper we focus on upper and lower bounds for approximating the problem.1.1Problem definition and preliminariesWe now describe the basic version of our problem.We consider a network and a set of demands D where each demand i is routed on a given path P i.We require that each demand is assigned a wavelengthλfrom the set{0,1,...,µ−1}.For each link e,if at most r e demands passing through link e are assigned wavelength λfor eachλ,then the number offibers required on link e is r e.Ifℓe is the number of paths that pass through e,then f e=ℓe/µis clearly a lower bound on r e.There are a number of distinct ways to define the objective function.For the reasons mentioned earlier we focus on a variant in which our goal is to minimize the maximum ratio between the number offibers deployed on a linke and the corresponding lower boundf e.(We mention some other variants in Section5.)The problem may be formulated as an integer program.Let variable C i,λindicate whether or not demand i uses wavelengthλ.Our problem,which we call Min-Fiber,can be written as follows for binary C i,λ.min zsubject toi:e∈P i C i,λ≤z·f e∀e,λ(1)λC i,λ=1∀i(2)We note that the linear relaxation of the above IP always has an optimal solution z=1and C i,λ=1/µfor all demands i and wavelengthsλ.1.2Our Results–We begin in Section2by presenting a negative result.We show that unless NP⊆ZPP there is no polynomial-time constant-factor approximation algo-rithm for the Min-Fiber problem.ZPP is the class of languages that can be recognized using a randomized algorithm that always gives the correct answer and whose expected running time is polynomial in the size of the input.Our result is based on the hardness result for graph coloring of Feige and Kilian[9].–In Section3we further improve the lower bound.Unless all languages in NP have randomized algorithms with running time O(n polylog(n)),we show that there is no logγµ-approximation for anyγ∈(0,1)and no logγm-approximation for anyγ∈(0,0.5)where m is the number of links in the network.–In Section4we turn our attention to positive results.In Section4.1we show that using randomized rounding we can obtain a solution in which the number offibers required on each link e is at most2f e+6(log m+ logµ).(All logarithms are to the base e.)This gives us an O(log m+logµ) approximation algorithm.We note that this algorithm can be derandomized using the standard method of conditional expectations.In Section4.2we apply the path-length rounding scheme of[12]to createa solution in which the number offibers required on each link e is at mostf e+D max,where D max is the length of the longest path in the network.Thisgives us an O(D max)approximation algorithm which is an improvement over the randomized rounding method when the paths are short.In the full version of the paper[2]we apply a constructive version of the Lov´a sz Local Lemma to obtain a randomized algorithm with approximation ratio O(log D max+logµ)and polynomial expected running time.–In Section5we conclude by presenting two variants of the Min-Fiber prob-lem and indicating which of our results still apply.1.3Previous WorkFor the case in which the number of available wavelengths is notfixed,the problem of minimizing the number of wavelengths used has been much stud-ied,e.g.[1,3,4,21].Some papers focus on common special topologies such as rings[14,24]and trees[16,15,7].The work listed here is by no means complete.A good survey on the subject can be found in[13].Our problem offiber minimization with afixedfiber capacity has been in-troduced more recently.In[25,18]the authors prove that coloring demands on a line only requires the minimum number offibers per link,i.e.⌈f e⌉fibers on link e.This generalizes the well-known algorithm for coloring interval graphs. In addition,[18]shows that the problem becomes NP-hard once the network topology is more complicated.The authors provide2-approximation algorithms for rings and stars.Recent work on trees include[6,8]and the results in[6] imply a4-approximation.For a general network topology,[23]uses randomized rounding to obtain an approximation algorithm for the variant of the problem in which the aim is to minimize the total amount offiber deployed.2Basic Lower BoundIn this section we show that there is no constant factor approximation to the Min-Fiber problem unless NP⊆ZPP.Our construction is based on hardness of approximation results for graph coloring.For any graph G we useχ(G)to denote the chromatic number of G andα(G)to denote the size of the maximum independent set of G.Throughout this section we shall use the terms“color”and“wavelength”interchangeably.Feige and Kilian[9]construct a randomized reduction from3SAT to graph coloring with the following properties.Given a3CNF formulaϕand a constant ε,they randomly construct an n-node graph G(where n is polynomial in the size ofϕ)such that,–Ifϕis satisfiable then with probability1,G can be colored with nεcolors,i.e.χ(G)≤nε.–Ifϕis not satisfiable then with high probability the maximum independent set in G has at most nεnodes,i.e.α(G)≤nεwith high probability.Note that sinceα(G)·χ(G)≥n this immediately implies thatχ(G)≥n1−ε. Feige and Kilian use this reduction to show that there is no n1−εapproximation for graph coloring unless NP⊆ZPP.We shall use it to show that for any constantc there is no c-approximation for Min-Fiber unless NP⊆ZPP.2.1Constructing an instance of Min-FiberWe now demonstrate how to take a graph G and create an instance of Min-Fiber on a network N.For each node v in G we have a demand d v.The links in N consist of two sets E1and E2.All links in E1are non-adjacent,i.e.no2links in E 1have a vertex in common.The links in E 2are used to connect up the links in E 1.More precisely,for each clique Q in G with c +1nodes we create a link e Q in N and these links form the link set E 1.The demand d v passes through e Q for all v ∈Q .If demand d v has to pass through links e Q 0,...,e Q z −1then there also exists a link f v,j in E 2that connects the head of e Q j with the tail of e Q j +1.The full path of d v is e Q 0,f v,0,e Q 1,...,e Q z −2,f v,z −2,e Q z −1.We illustrate the construction of the network N from a graph G in Figure 1.The number of colors in our instance of Min-Fiber is µ=n ε.31267541d 2d 3d 4d d 2d 37d 1d d 5d 6Fig.1.An example of the construction for c =2.(Left)Graph G with 4cliques of size3.(Upper right)Demands and routes created from G .(Lower right)Network N ,solid lines represent links in E 1and dotted lines represent those in E 2.2.2Reduction from 3SAT to Min-FiberGiven a 3CNF formula ϕwe first choose a constant εsuch that ε<1c +1.We then construct a random n -node graph G according to the method of Feige andKilian [9]for this parameter ε.Finally,we convert the graph G into an instance of Min-Fiber on a network N according to the method of the previous section.Note that since c is a constant,the number of demands and links in N are both polynomial in n which is in turn polynomial in the size of ϕ.Lemma 1.If ϕis satisfiable then with probability 1the demands in N can be colored such that at most one fiber is required on each link.If ϕis not satisfiable then with high probability,for any coloring of the demands in N ,some link requires c +1fibers.Proof.Suppose that ϕis satisfiable.Then with probability 1the graph G is colorable with µ=n εcolors.For any such coloring,we color the demands in N such that demand d v receives the same color as node v .Clearly,for any clique Q in G and any color λ,there is at most one node in Q that receives color λ.Hence for any link e Q in E 1,there is at most one demand passing through linke Q that receives colorλ.Therefore each link in E1requires only onefiber in order to carry all its demands.The links in E2have only one demand and so they trivially require onefiber only.Hence at most onefiber is required on any link in N.To prove the other direction,suppose thatϕis unsatisfiable.Then with high probabilityα(G)≤nε.Suppose for the purpose of contradiction that we can color the demands in N withµ=nεcolors such that each link requires at most cfibers.This implies that for any link e Q in E1,not all the demands passing through e Q receive the same color.Consider now the corresponding coloring of the nodes in G.1By the construction of our network N,for any clique Q with c+1nodes,not every node in Q receives the same color.Let X be the induced subgraph of G on the set of nodes that constitutes the largest color class.We have just shown that X does not contain a clique of size c+1.Moreover,since X is contained in G,α(X)≤α(G)≤nε.Ramsey’s theorem(see e.g.[19])immediately implies that,|X|≤ α(G)+(c+1)−2(c+1)−1 ≤α(G)c.(3) Since X constitutes the largest color class and there are nεcolors,|X|nε≥n. Hence,|X|≥n1−ε⇒α(G)c≥n1−ε⇒α(G)≥n1−εc>nε,.This contradicts the fact thatα(G)≤nε.sinceε<1c+1Theorem1.There is no c-approximation to Min-Fiber for any constant c unless NP⊆ZPP.Proof.Suppose for the purpose of contradiction that C is a polynomial time c-approximation algorithm.We use this to construct a randomized algorithm B for3SAT.For each instanceϕ,algorithm B creates a random graph G and then converts it to an instance of Min-Fiber on a network N as described above.It then runs algorithm C on the instance of Min-Fiber.If the solution returned by algorithm C is at most c then algorithm B returns“satisfiable”,otherwise algorithm B returns“unsatisfiable”.Lemma1implies that,–Ifϕis satisfiable then the optimal solution to the instance of Min-Fiber is1.Since algorithm C is a c-approximation algorithm,it returns a value of atmost c.Therefore algorithm B outputs“satisfiable”.–Ifϕis unsatisfiable then with high probability the optimal solution to the instance of Min-Fiber is c+1.Therefore algorithm C returns a solution of at least c+1.Therefore algorithm B outputs“unsatisfiable”.1Note that this is not necessarily a proper coloring.Some edges in G may have both endpoints assigned the same color.Note that algorithm B has one-sided error.Hence3SAT∈coRP and so NP⊆coRP.This implies RP⊆NP⊆coRP⊆coNP which in turn implies NP= coNP=RP=coRP=RP∩coRP=ZPP.3Improved Lower BoundIn this section we derive more general hardness results by examining the con-struction of Feige and Kilian in more detail.In particular,given a3CNF formula ϕand a constantε,they construct a random graph G on n nodes with parame-ters a,ρ,A and k.(As an aside,the parameters a,ρand A are associated with a randomized Probabilistically Checkable Proof for NP and k is associated with a random graph product on a graph generated from the PCP.However,these interpretations are not important for our purposes.)The parameters are chosen so that the following relationships hold.More specifically,the parameters a and ρarefixed to some constants such that(5)holds.The parameter A is polyno-mial in the size ofϕand k is polylogarithmic in the size ofϕ.In particular,k is chosen sufficiently large such that Lemma2holds.n=a k(4)1≥log aρlog a≥1−ε(5)A=poly(|ϕ|)(6)k=Θ(log1/δ|ϕ|)for anyδ∈(0,1)of our choice(7) Feige and Kilian show that Graph G has the following properties.1.Ifϕis satisfiable then with probability1,G can be colored with(1+log n)/ρkcolors,i.e.χ(G)≤(1+log n)/ρk.2.Ifϕis not satisfiable thenα(G)≤kA with high probability,which impliesχ(G)≥n/(kA).From the graph G we construct an instance of Min-Fiber in the same manner as in the previous section.The number of links m in the newly constructed network N is O(n c).We set,µ=(1+log n)/ρk(8)c=log1−δn for anyδ∈(0,1)of our choice(9) Lemma2.We can choose k=Θ(log1/δ|ϕ|)such that(1+log n)(kA)cρk<n. Proof.Immediate from the parameter definitions.The following is analogous to Lemma1.Lemma3.Ifϕis satisfiable then with probability1the demands in N can be colored withµcolors such that at most1fiber is required on each link.Ifϕis not satisfiable then with high probability,for any coloring of the demands in N, some link requires c+1fibers.Proof.For the case in whichϕis satisfiable,the proof is identical to Lemma1.For the other direction,suppose thatϕis unsatisfiable but we color the demands in N withµcolors such that each link requires at most cfibers.Consider the corresponding coloring of G and let X be the induced subgraph of G on the set of nodes that constitutes the largest color class.As in inequality(3)in the proof of Lemma1,|X|≤α(G)c.By the construction of G,with high probability α(G)≤kA,which implies|X|≤(kA)c.Since X constitutes the largest color class and there areµ=(1+log n)/ρk colors,|X|≥n/µ=nρk/(1+log n).These inequalities imply that(kA)c≥nρk/(1+log n)which contradicts Lemma(2).Note that since we have a link in the network N for each subset of c+1nodes in G,the size of the instance of Min-Fiber is polynomial in n c.The following is analogous to Theorem1.Theorem2.Unless3SAT has a randomized algorithm with expected running time O(|ϕ|polylog(|ϕ|)),there is no logγµ-approximation to Min-Fiber for any γ∈(0,1),and there is noΘ(logγm)-approximation for anyγ∈(0,0.5).Here,µis the number of colors perfiber and m is the number of links in Min-Fiber. Proof.As in Theorem1we assume for the purpose of contradiction that C is a polynomial time c-approximation algorithm where c is defined in(9).From C we can construct a randomized algorithm B for3SAT such that ifϕis satisfiable then B outputs“satisfiable”;ifϕis unsatisfiable then with high probability B outputs“unsatisfiable”.The correctness of B is identical to Theorem1.The running time of B is O(|ϕ|polylog(|ϕ|))since both k and c are polylogarithmic in|ϕ|.Sinceµ≤n and m=O(n c)we can show that c>(logµ)1−δand c=Ω((log m)1−1/(2−δ)).We note that B can give an incorrect answer with low probability.However,in the same way that NP⊆coRP implies NP⊆ZPP we can convert B into a randomized algorithm that always gives the correct answer and whose expected running time is O(|ϕ|polylog(|ϕ|)).4Upper Bounds4.1Randomized RoundingRecall that the linear relaxation of the our Min-Fiber problem always has an optimal solution z=1and C i,λ=1/µfor all demands i and wavelengthsλ. We adopt the technique of randomized rounding introduced in[20].For each demand i we choose a number x i uniformly at random in the range[0,1].If x i∈[k/µ,(k+1)/µ)then we round C i,λto1forλ=k and round C i,λto0 forλ=k.After rounding the constraint(2)still holds.We use the ChernoffBound[17]to see how much constraint(1)is violated.LetˆC i,λdenote the rounded solution.[ChernoffBound]If X 1,...,X n are independent binary random variables where the expectation x =E [ i X i ],then it holds for all δ>0that,Pr [i X i ≥(1+δ)x ]≤e −min(δ2,δ)·x/3.Lemma 4.For a particular link e and wavelength λ,Pr i :e ∈P i ˆC i,λ≥2f e ≤m −2µ−2if f e ≥6(log m +log µ),Pr i :e ∈P i ˆC i,λ≥f e +6(log m +log µ)≤m −2µ−2if f e <6(log m +log µ).Proof.By definition,the expected value of E [ˆC i,λ]is 1/µ.Hence,E i :e ∈P i ˆC i,λ =f e .Note that for a fixed link e and wavelength λ,the rounding of variables C i,λfor demands i that go through e are independent events.We can therefore apply the ChernoffBound.If f e ≥6(log m +log µ),thenPr i :e ∈P i ˆC i,λ≥(1+1)f e ≤e−f e /3≤e −2log m −2log µ=m −2µ−2.If f e <6(log m +log µ),thenPr i :e ∈P i ˆC i,λ≥ 1+1f e ·6(log m +log µ) f e ≤e−2log m −2log µ=m −2µ−2.By applying the union bound over all links and wavelengths,we obtain the following.Theorem 3.We can round the fractional optimal solution such that with high probability the number of fibers deployed on each link e is at most 2f e +O (log m +log µ).This implies an O (log m +log µ)approximation algorithm.We note that this algorithm can be derandomized by the standard method of conditional probabilities.We also note that for large values of f e the approxi-mation ratio approaches stly,we remark that by using the slightly tighter Chernoffbound P r [ i X i ≥(1+δ)x ]≤(e δ/(1+δ)1+δ)x ,the approximationratio can be marginally improved to O (log m log log m +log µlog log µ).However,for ease ofexposition we typically ignore “log log”factors in this paper.In the full version of the paper [2]we apply a constructive version of the Lov´a sz Local Lemma (see for example Theorem 3.84of [22])to obtain a ran-domized algorithm with polynomial expected running time and approximation ratio O (log D max +log µ),where D max is the maximum number of links along any demand path.In many optical networks D max is significantly smaller than m .We omit the proof from this version in the interests of space.Theorem 4.We can round the fractional optimal solution such that the number of fibers deployed on each link e is at most 2f e +6(log D max +log µ).4.2Path Length RoundingThe following rounding theorem is due to Karp,Leighton,Rivest,Thompson, Vazirani and Vazirani[12].[KLRTVV Rounding Theorem]Let A be a real-valued r×s matrix and let x be a real-valued s-vector,let b be a real-valued r-vector such that Ax=b and let∆be a positive real number such that in every column of A,1.the column sum of the positive elements is at most∆,and2.the column sum of the negative elements is at least−∆.Then we can compute an integral s-vectorˆx such that,1.ˆx is a rounded version of x,i.e.ˆx i=⌊x i⌋orˆx i=⌈x i⌉for1≤i≤s,and2.Aˆx=ˆb whereˆb i−b i≤∆for all1≤i≤r.In the case that all entries in Aand b are integers,then a stronger bound applies:ˆb i−b i≤∆−1.It is easy to see that matrix A in the LP formulation of Min-Fiber has0/1 entries and its column sum is upper bounded by the longest path length plus1, i.e.max i|P i|+1.By applying the KLRTVV Rounding Theorem,we obtain, Theorem5.We can round the fractional optimal solution such that the number offibers deployed on each link e is at most f e+D max.5ConclusionsIn this paper we have presented positive and negative results for approximating the Min-Fiber problem.We conclude by briefly discussing two variants of Min-Fiber with different objective functions and seeing how our results apply.In the basic Min-Fiber problem the objective is to minimize the ratio between the number offibers deployed on link e and the lower bound f e.For the sake of comparison,we restate the integer program.Basic Versionmin zsubject to i:e∈P i C i,λ≤z·f e∀e,λλC i,λ=1∀iIn thefirst variant the new objective is to minimize the maximum,over all links e,of the number offibers used on link e.As an integer program,this variant may be written as,Variant1min zsubject to i:e∈P i C i,λ≤z∀e,λλC i,λ=1∀iWe note that the hardness results of Sections2and3follow through,e.g.there is no constant-factor approximation for Variant1of Min-Fiber unless NP⊆ZPP. This is because for the case in which the3CNF formulaφis satisfiable,all links in the network require exactly1fiber.We also note that a lower bound on the optimal value of this problem is max e f e.By concentrating on the link e with the maximum value of f e,it is not hard to see that the approximation ratios proved in Section4also hold for this variant.In the second variant we assume that we somehow know the cost perfiber on link e.We denote this cost by L e.Our objective is to minimize the total cost offiber needed to carry all the demands.We can formulate this variant as the following integer program.Variant2min e z e L esubject to i:e∈P i C i,λ≤z∀e,λλC i,λ=1∀iOnce again,the approximation ratios proved in Sections4apply to this vari-ant.Furthermore,it can be shown that randomized rounding actually gives an O(logµ)approximation for this variant[5].However,our hardness results of Sections2and3no longer apply.Indeed,for the instances constructed in our reductions,randomized rounding gives a constant factor approximation for the problem of minimizing the totalfiber length.AcknowledgementThe authors wish to thank Chandra Chekuri,Bruce Shepherd and the anony-mous referees for many helpful comments.References1. 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