An approach to Symmetry Breaking in Distributed Constraint Satisfaction Problems

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感受数学之美的给孩子看的英文书

感受数学之美的给孩子看的英文书

感受数学之美的给孩子看的英文书全文共3篇示例,供读者参考篇1Title: Exploring the Beauty of MathematicsIntroductionMathematics is more than just numbers and equations, it is a fascinating and intricate puzzle that challenges our minds and shapes the world around us. In this book, we will delve into the beauty of mathematics and explore its endless possibilities. Through engaging stories, colorful illustrations, and interactive activities, children will discover the magic of numbers and the wonders of geometry, algebra, and more.Chapter 1: The Power of PatternsFrom the mesmerizing spiral of a seashell to the symmetrical petals of a flower, patterns are everywhere in nature. In this chapter, children will learn how to recognize and create patterns using basic shapes and colors. Through hands-on activities such as drawing and coloring, they will develop a keen eye for symmetry and repetition.Chapter 2: The Joy of GeometryGeometry is the study of shapes and their properties, and it is the foundation of many mathematical concepts. In this chapter, children will explore the world of polygons, circles, and angles. They will learn how to measure and calculate areas and perimeters, and discover the beauty of tessellations and fractals.Chapter 3: The Wonder of NumbersNumbers are the building blocks of mathematics, and they hold endless mysteries waiting to be uncovered. In this chapter, children will learn about the history of numbers, from the ancient civilizations to modern mathematicians. They will explore the concepts of prime numbers, fractions, and decimals, and engage in fun games and puzzles to sharpen their numerical skills.Chapter 4: The Magic of AlgebraAlgebra is the language of equations and variables, and it is crucial for solving complex problems. In this chapter, children will embark on a journey through algebraic expressions, equations, and inequalities. They will learn how to simplify expressions, solve equations, and graph functions, giving them the tools to tackle real-world challenges with confidence.Chapter 5: The Beauty of CalculusCalculus is the study of change and motion, and it is a powerful tool for understanding the world around us. In this chapter, children will be introduced to the concepts of derivatives, integrals, and limits. They will explore the connection between calculus and physics, biology, and other sciences, and witness the beauty of mathematical modeling in action.ConclusionMathematics is a treasure trove of beauty and wonder, waiting to be explored by curious minds. By diving into the world of patterns, geometry, numbers, algebra, and calculus, children can unlock the secrets of the universe and unleash their creativity and problem-solving skills. This book is just the beginning of their mathematical journey, and I hope it inspires them to continue exploring the infinite possibilities of this fascinating field.篇2Title: Exploring the Beauty of Mathematics: A Book for ChildrenIntroductionMathematics is a beautiful and fascinating subject that is often misunderstood and feared by many children. However, it isessential to teach children about the beauty and wonders of mathematics from a young age to foster a love and appreciation for the subject. This book aims to introduce children to the beauty of mathematics in a fun and engaging way, helping them see the world through the lens of mathematics.Chapter 1: The Magic of NumbersIn this chapter, children will learn about the magic of numbers and how they are used in everyday life. From counting to discovering patterns and sequences, numbers are all around us. Children will explore the concept of symmetry, prime numbers, and the Fibonacci sequence, opening their minds to the beauty of mathematics.Chapter 2: The Language of ShapesShapes are everywhere, from the geometry of buildings to the symmetry of nature. In this chapter, children will learn about different geometric shapes, such as circles, squares, triangles, and polygons. They will discover the beauty of symmetry and tessellations, as well as the concept of fractals and the golden ratio.Chapter 3: The Art of Problem SolvingMathematics is not just about numbers and shapes but also about problem-solving. In this chapter, children will learn about different problem-solving strategies, such as breaking down a problem, looking for patterns, and using logical reasoning. They will explore puzzles, riddles, and games that challenge their minds and nurture their problem-solving skills.Chapter 4: The Power of PatternsPatterns are an essential part of mathematics, helping us make sense of the world around us. In this chapter, children will learn about different types of patterns, such as number patterns, shape patterns, and symmetry. They will discover how patterns are used in mathematics, art, music, and nature, showing them the interconnectedness of the world.Chapter 5: The Beauty of InfinityThe concept of infinity is both mind-boggling and beautiful. In this chapter, children will learn about different types of infinity, such as countable and uncountable infinity. They will explore the concept of limits, sequences, and series, as well as the infinite nature of fractals and the Mandelbrot set. Children will be amazed by the endless possibilities of infinity and its presence in mathematics and beyond.ConclusionMathematics is a subject full of wonder, beauty, and creativity. By introducing children to the beauty of mathematics at a young age, we can help them develop a love and appreciation for the subject. This book aims to inspire children to see the world through the lens of mathematics, encouraging them to explore, discover, and create with confidence and curiosity. Let's unlock the beauty of mathematics together and open the doors to endless possibilities.篇3Title: Discovering the Beauty of Mathematics: A Children's BookIntroduction:Mathematics is often seen as a difficult and intimidating subject, but in reality, it is a beautiful and fascinating field of study. Through this children's book, we aim to help young readers discover the beauty of mathematics and develop a deeper appreciation for the subject.Chapter 1: Introduction to MathematicsIn this chapter, we introduce the basic concepts of mathematics, such as numbers, shapes, and patterns. We explain how mathematics is all around us, from the natural world to the technology we use every day.Chapter 2: The Beauty of SymmetrySymmetry is a key concept in mathematics and can be found in nature, art, and architecture. In this chapter, we explore different types of symmetry and how they can be used to create beautiful designs.Chapter 3: Exploring PatternsMathematics is all about finding and understanding patterns. In this chapter, we look at different types of patterns, such as geometric patterns, number patterns, and fractals. We show how patterns can be both simple and complex, and how they can be found in nature and art.Chapter 4: The Magic of NumbersNumbers are the building blocks of mathematics, and they have many fascinating properties. In this chapter, we explore the beauty of numbers, from prime numbers to Fibonacci sequences. We also look at how numbers are used in everyday life, from telling time to measuring distances.Chapter 5: The Language of MathematicsMathematics has its own language, with symbols and equations that help us solve problems and communicate ideas. In this chapter, we introduce young readers to some basic mathematical symbols and show how they are used in equations.Chapter 6: The World of ShapesGeometry is a branch of mathematics that studies shapes and their properties. In this chapter, we explore different types of shapes, such as polygons, circles, and solids. We also look at how shapes are used in art and design.Conclusion:By the end of this book, we hope that young readers will have a better understanding of the beauty of mathematics and be inspired to explore the subject further. Mathematics is not just about solving equations - it is a way of thinking and seeing the world in a new light. We encourage children to embrace the beauty of mathematics and enjoy the journey of discovery that it offers.。

Symmetry breaking in graphs

Symmetry breaking in graphs
1 2 0 1 2 1 0 1 3 4 5 0 1 2 3 1 1
the electronic journal of combinatorics 3 (1996), #R18
3
Aut(Gn) = Sn. In an r-distinguishing labeling, each of the pairs consisting of a vertex of the clique and its pendant neighbor must have a di erent ordered pair of labels; there are r possible ordered pairs of labels using r p colors, hence D(Gn) = d n e. On the other hand, recall that the in ation of graph G, Inf (G), is de ned as follows: the vertices of Inf (G) consist of ordered pairs of elements from G, the rst being a vertex and the second an edge incident to that vertex. Two vertices in Inf (G) are adjacent if they di er in exactly one component 3]. In the context of polyhedra, the in ation of a graph is also known as the truncation 4]. Label the vertices of Kn with 1; : : : ; n. Then vertices of Inf (Kn) can be labelled fij j1 i n; 1 j n; and i 6= j g in the obvious way. Assigning the color 1 to vertex ij if i < j , and the color 2 otherwise shows that D(Inf (Kn)) = 2. It is easy to see that Aut(Inf (Kn)) = Sn, provided that n 4.

symmetric 名词

symmetric 名词

Symmetric1. IntroductionSymmetric is a term used in mathematics and other fields to describe objects or concepts that possess a certain type of symmetry. In mathematics, symmetry refers to a property where an object remains unchanged under certain transformations, such as reflection, rotation, or translation. In this article, we will explore the concept of symmetry and its various applications in different disciplines.2. Symmetry in MathematicsSymmetry plays a fundamental role in mathematics and is widely studied in various branches, including geometry, algebra, and group theory. In geometry, symmetric objects are those that can be divided into two or more parts that are mirror images of each other. For example, a circle is symmetric with respect to any line passing through its center.Symmetry can also be observed in patterns and shapes. Regular polygons such as squares and equilateral triangles possess rotational symmetry because they can be rotated by certain angles without changing their appearance. Fractals, which are intricate mathematical patterns that repeat at different scales, often exhibit self-similarity and possess various types of symmetries.In algebra, symmetry is explored through the concept of functions. A function is said to be symmetric if it satisfies the condition f(x) =f(-x) for all values of x in its domain. This property implies that the graph of the function is symmetric with respect to the y-axis.Group theory provides a rigorous framework for studying symmetry by defining mathematical structures called groups. A group consists of a set of elements and an operation that combines two elements to produce another element in the set. Symmetry groups describe all possible symmetries of an object or system and play a vital role in understanding its properties.3. Symmetry in PhysicsSymmetry has profound implications in physics and is essential for understanding the laws of nature. The principle of symmetry lies at theheart of many fundamental theories, such as classical mechanics, quantum mechanics, and general relativity.In classical mechanics, the conservation of angular momentum is a consequence of rotational symmetry. The laws of motion remain the same regardless of the direction in which an object is oriented. This symmetry is evident in everyday life, where the behavior of objects under different orientations follows consistent patterns.In quantum mechanics, symmetry plays a crucial role in determining the behavior of particles and their interactions. The principles of quantum field theory rely heavily on the concept of gauge symmetry, which describes the invariance of physical laws under certain transformations. Symmetries such as time translation symmetry and particle-antiparticle symmetry are fundamental to our understanding of elementary particles and their interactions.General relativity, Einstein’s theory of gravity, incorporates the principle of general covariance, which states that physical laws should be independent of the choice of coordinates. This symmetry reflects the idea that space and time are not absolute but rather depend on the observer’s frame of reference.4. Symmetry in BiologySymmetry is prevalent in biology and plays a crucial role in understanding various biological processes and structures. Many organisms exhibit bilateral symmetry, where their bodies can be divided into two mirror-image halves along a plane. This type of symmetry is observed in animals ranging from insects to mammals.Bilateral symmetry provides advantages such as improved mobility and sensory perception. It allows for efficient movement by dividing body parts into corresponding pairs such as legs or wings. It alsofacilitates better coordination between sensory organs located on opposite sides of an organism.Symmetry is also observed at smaller scales within organisms. For example, DNA molecules possess helical symmetry due to their double-stranded structure. Proteins often exhibit internal symmetries that influence their folding patterns and functions.Studying symmetric patterns in nature can provide insights into evolutionary processes and ecological relationships between differentspecies. Understanding how symmetrical structures arise and function can help biologists unravel complex biological systems.5. Symmetry in Art and DesignSymmetry has been a fundamental principle in art and design for centuries. Artists and designers often use symmetrical patterns and compositions to create aesthetically pleasing and visually balanced works.Symmetry can be found in various art forms, including painting, sculpture, architecture, and textiles. The use of bilateral symmetry can create a sense of harmony and orderliness. Radial symmetry, where elements are arranged around a central point, is also frequently employed to achieve balance and visual interest.In modern design, the concept of symmetry has evolved to include asymmetrical compositions as well. Asymmetry introduces a dynamic element by intentionally breaking traditional symmetrical arrangements. This approach adds visual tension and can create a more engaging and thought-provoking experience for the viewer.6. ConclusionSymmetry is a fascinating concept that permeates many aspects of our world, from mathematics to physics, biology, and art. It represents an inherent orderliness and balance that is both aesthetically pleasing and intellectually stimulating.The study of symmetry has led to significant advancements in various fields, providing insights into the fundamental laws of nature, the structure of biological systems, and the principles of design. By understan ding symmetry’s underlying principles and exploring its applications, we gain a deeper appreciation for the intricate patterns that surround us.。

2020年高考英语江苏省名师押题密卷及解析四

2020年高考英语江苏省名师押题密卷及解析四

江苏省2020年高考英语名师押题密卷(4)第一部分听力(共两节,满分20分)略第二部分英语知识运用(共两节,满分35分)第一节单项填空(共15小题;每小题1分,满分15分)请认真阅读下面各题,从题中所给的A、B、C、D四个选项中,选出最佳选项。

21.Teachers have to constantly update their knowledge in order to maintain their professional_______.A. consequenceB. independenceC. competenceD. intelligence22.—Why do you suggest we buy a new machine?—Because the old one has been damaged_______.A. beyond reachB. beyond repairC. beyond controlD. beyond description23.You may not have played very well today, but at least you’ve got through to the next round and_______.A. tomorrow never comesB. tomorrow is another dayC. never put off till tomorrowD. there is no tomorrow24.Nine in ten parents saidthere were significant differences in their approach to educating theirchildren compared with_______ of their parents.A. thoseB. oneC. bothD. that25.In that school, English is compulsory for all students, but French and Russian are_______.A. specialB. regionalC. optionalD. original26.—Hi, Torry, can I use your computer for a while this afternoon?—Sorry._______.A. It’s repairedB. It has been repairedC. It’s being repairedD. It had been repaired27.The Science Museum,_______ we visited during a recent trip to Britain, is one of London’s tourist attractions.A. whichB. whatC. thatD. where28.It was never clear_______the man hadn’t reported the accident sooner.A. thatB. howC. whenD. why29.The fact that so many people still smoke in public places_______that we may needa nationwide campaign to raise awareness of the risks of smoking.A. suggestB. suggestsC. suggestedD. suggesting30.It sounds like something is wrong with the car's engine._______, we’d better take it to the garage immediately.A. OtherwiseB. If notC. But for thatD. If so31.In order to offer their children a better education, many parents will send themto college ____ it takes, even if that means a huge amount of debt.A.whatB. thatC. whateverD. however32. a diary every day and you’ll improve your writing.A. KeepingB. To keepC. KeepD. If you keep33. the news, so far, has been good, there may be bad days ahead.A. WhenB. WhileC. IfD. Since34. So far as I know, more than one person _______connected with the accident.A. isB. hasC. areD. have35.Paris serves both as the political center of the nation and as_______.A. the cultural center alsoB. being a cultural centerC. to be a center of cultural activityD. a center of cultural activity第二节完形填空(共20小题;每小题1分,满分20分)请认真阅读下面短文,从短文后各题所给的A、B、C、D四个选项中,选出最佳选项。

Sets of symmetry breaking constraints

Sets of symmetry breaking constraints
3 Examples of Symmetry Breaking
Constraints
In this section, two examples are given to show that different variable orders do not necessarily yield different constraints, but may do.
broken with a small number of constraints (linear in the number of variables) and gives a procedure for generating them from the symmetry group. Here, the procedure is adapted to generate all the symmetrically distinct sets of constraints. As in [Puget, 2004], instances of the ‘graceful graph’ problem are used as examples, since these do have variable symmetry and an allDifferent constraint on the variables. Graceful graph problems also have a value symmetry, but for the present purposes that is ignored.
Sets of Symmetry Breaking Constraints
Barbara M. Smith Cork Constraint Computation Centre, University College Cork, Ireland

Singularity of the density of states in the two-dimensional Hubbard model from finite size

Singularity of the density of states in the two-dimensional Hubbard model from finite size

a r X i v :c o n d -m a t /9503139v 1 27 M a r 1995Singularity of the density of states in the two-dimensional Hubbard model from finitesize scaling of Yang-Lee zerosE.Abraham 1,I.M.Barbour 2,P.H.Cullen 1,E.G.Klepfish 3,E.R.Pike 3and Sarben Sarkar 31Department of Physics,Heriot-Watt University,Edinburgh EH144AS,UK 2Department of Physics,University of Glasgow,Glasgow G128QQ,UK 3Department of Physics,King’s College London,London WC2R 2LS,UK(February 6,2008)A finite size scaling is applied to the Yang-Lee zeros of the grand canonical partition function for the 2-D Hubbard model in the complex chemical potential plane.The logarithmic scaling of the imaginary part of the zeros with the system size indicates a singular dependence of the carrier density on the chemical potential.Our analysis points to a second-order phase transition with critical exponent 12±1transition controlled by the chemical potential.As in order-disorder transitions,one would expect a symmetry breaking signalled by an order parameter.In this model,the particle-hole symmetry is broken by introducing an “external field”which causes the particle density to be-come non-zero.Furthermore,the possibility of the free energy having a singularity at some finite value of the chemical potential is not excluded:in fact it can be a transition indicated by a divergence of the correlation length.A singularity of the free energy at finite “exter-nal field”was found in finite-temperature lattice QCD by using theYang-Leeanalysisforthechiral phase tran-sition [14].A possible scenario for such a transition at finite chemical potential,is one in which the particle den-sity consists of two components derived from the regular and singular parts of the free energy.Since we are dealing with a grand canonical ensemble,the particle number can be calculated for a given chem-ical potential as opposed to constraining the chemical potential by a fixed particle number.Hence the chem-ical potential can be thought of as an external field for exploring the behaviour of the free energy.From the mi-croscopic point of view,the critical values of the chemical potential are associated with singularities of the density of states.Transitions related to the singularity of the density of states are known as Lifshitz transitions [15].In metals these transitions only take place at zero tem-perature,while at finite temperatures the singularities are rounded.However,for a small ratio of temperature to the deviation from the critical values of the chemical potential,the singularity can be traced even at finite tem-perature.Lifshitz transitions may result from topological changes of the Fermi surface,and may occur inside the Brillouin zone as well as on its boundaries [16].In the case of strongly correlated electron systems the shape of the Fermi surface is indeed affected,which in turn may lead to an extension of the Lifshitz-type singularities into the finite-temperature regime.In relating the macroscopic quantity of the carrier den-sity to the density of quasiparticle states,we assumed the validity of a single particle excitation picture.Whether strong correlations completely distort this description is beyond the scope of the current study.However,the iden-tification of the criticality using the Yang-Lee analysis,remains valid even if collective excitations prevail.The paper is organised as follows.In Section 2we out-line the essentials of the computational technique used to simulate the grand canonical partition function and present its expansion as a polynomial in the fugacity vari-able.In Section 3we present the Yang-Lee zeros of the partition function calculated on 62–102lattices and high-light their qualitative differences from the 42lattice.In Section 4we analyse the finite size scaling of the Yang-Lee zeros and compare it to the real-space renormaliza-tion group prediction for a second-order phase transition.Finally,in Section 5we present a summary of our resultsand an outlook for future work.II.SIMULATION ALGORITHM AND FUGACITY EXPANSION OF THE GRAND CANONICALPARTITION FUNCTIONThe model we are studying in this work is a two-dimensional single-band Hubbard HamiltonianˆH=−t <i,j>,σc †i,σc j,σ+U i n i +−12 −µi(n i ++n i −)(1)where the i,j denote the nearest neighbour spatial lat-tice sites,σis the spin degree of freedom and n iσis theelectron number operator c †iσc iσ.The constants t and U correspond to the hopping parameter and the on-site Coulomb repulsion respectively.The chemical potential µis introduced such that µ=0corresponds to half-filling,i.e.the actual chemical potential is shifted from µto µ−U412.(5)This transformation enables one to integrate out the fermionic degrees of freedom and the resulting partition function is written as an ensemble average of a product of two determinantsZ ={s i,l =±1}˜z = {s i,l =±1}det(M +)det(M −)(6)such thatM ±=I +P ± =I +n τ l =1B ±l(7)where the matrices B ±l are defined asB ±l =e −(±dtV )e −dtK e dtµ(8)with V ij =δij s i,l and K ij =1if i,j are nearestneigh-boursand Kij=0otherwise.The matrices in (7)and (8)are of size (n x n y )×(n x n y ),corresponding to the spatial size of the lattice.The expectation value of a physical observable at chemical potential µ,<O >µ,is given by<O >µ=O ˜z (µ){s i,l =±1}˜z (µ,{s i,l })(9)where the sum over the configurations of Ising fields isdenoted by an integral.Since ˜z (µ)is not positive definite for Re(µ)=0we weight the ensemble of configurations by the absolute value of ˜z (µ)at some µ=µ0.Thus<O >µ= O ˜z (µ)˜z (µ)|˜z (µ0)|µ0|˜z (µ0)|µ0(10)The partition function Z (µ)is given byZ (µ)∝˜z (µ)N c˜z (µ0)|˜z (µ0)|×e µβ+e −µβ−e µ0β−e −µ0βn (16)When the average sign is near unity,it is safe to as-sume that the lattice configurations reflect accurately thequantum degrees of freedom.Following Blankenbecler et al.[1]the diagonal matrix elements of the equal-time Green’s operator G ±=(I +P ±)−1accurately describe the fermion density on a given configuration.In this regime the adiabatic approximation,which is the basis of the finite-temperature algorithm,is valid.The situa-tion differs strongly when the average sign becomes small.We are in this case sampling positive and negative ˜z (µ0)configurations with almost equal probability since the ac-ceptance criterion depends only on the absolute value of ˜z (µ0).In the simulations of the HSfields the situation is dif-ferent from the case of fermions interacting with dynam-ical bosonfields presented in Ref.[1].The auxilary HS fields do not have a kinetic energy term in the bosonic action which would suppress their rapidfluctuations and hence recover the adiabaticity.From the previous sim-ulations on a42lattice[3]we know that avoiding the sign problem,by updating at half-filling,results in high uncontrolledfluctuations of the expansion coefficients for the statistical weight,thus severely limiting the range of validity of the expansion.It is therefore important to obtain the partition function for the widest range ofµ0 and observe the persistence of the hierarchy of the ex-pansion coefficients of Z.An error analysis is required to establish the Gaussian distribution of the simulated observables.We present in the following section results of the bootstrap analysis[17]performed on our data for several values ofµ0.III.TEMPERATURE AND LATTICE-SIZEDEPENDENCE OF THE YANG-LEE ZEROS The simulations were performed in the intermediate on-site repulsion regime U=4t forβ=5,6,7.5on lat-tices42,62,82and forβ=5,6on a102lattice.The ex-pansion coefficients given by eqn.(14)are obtained with relatively small errors and exhibit clear Gaussian distri-bution over the ensemble.This behaviour was recorded for a wide range ofµ0which makes our simulations reli-able in spite of the sign problem.In Fig.1(a-c)we present typical distributions of thefirst coefficients correspond-ing to n=1−7in eqn.(14)(normalized with respect to the zeroth power coefficient)forβ=5−7.5for differ-entµ0.The coefficients are obtained using the bootstrap method on over10000configurations forβ=5increasing to over30000forβ=7.5.In spite of different values of the average sign in these simulations,the coefficients of the expansion(16)indicate good correspondence between coefficients obtained with different values of the update chemical potentialµ0:the normalized coefficients taken from differentµ0values and equal power of the expansion variable correspond within the statistical error estimated using the bootstrap analysis.(To compare these coeffi-cients we had to shift the expansion by2coshµ0β.)We also performed a bootstrap analysis of the zeros in theµplane which shows clear Gaussian distribution of their real and imaginary parts(see Fig.2).In addition, we observe overlapping results(i.e.same zeros)obtained with different values ofµ0.The distribution of Yang-Lee zeros in the complexµ-plane is presented in Fig.3(a-c)for the zeros nearest to the real axis.We observe a gradual decrease of the imaginary part as the lattice size increases.The quantitative analysis of this behaviour is discussed in the next section.The critical domain can be identified by the behaviour of the density of Yang-Lee zeros’in the positive half-plane of the fugacity.We expect tofind that this density is tem-perature and volume dependent as the system approaches the phase transition.If the temperature is much higher than the critical temperature,the zeros stay far from the positive real axis as it happens in the high-temperature limit of the one-dimensional Ising model(T c=0)in which,forβ=0,the points of singularity of the free energy lie at fugacity value−1.As the temperature de-creases we expect the zeros to migrate to the positive half-plane with their density,in this region,increasing with the system’s volume.Figures4(a-c)show the number N(θ)of zeros in the sector(0,θ)as a function of the angleθ.The zeros shown in thesefigures are those presented in Fig.3(a-c)in the chemical potential plane with other zeros lying further from the positive real half-axis added in.We included only the zeros having absolute value less than one which we are able to do because if y i is a zero in the fugacity plane,so is1/y i.The errors are shown where they were estimated using the bootstrap analysis(see Fig.2).Forβ=5,even for the largest simulated lattice102, all the zeros are in the negative half-plane.We notice a gradual movement of the pattern of the zeros towards the smallerθvalues with an increasing density of the zeros nearθ=πIV.FINITE SIZE SCALING AND THESINGULARITY OF THE DENSITY OF STATESAs a starting point for thefinite size analysis of theYang-Lee singularities we recall the scaling hypothesis forthe partition function singularities in the critical domain[11].Following this hypothesis,for a change of scale ofthe linear dimension LLL→−1),˜µ=(1−µT cδ(23)Following the real-space renormalization group treatmentof Ref.[11]and assuming that the change of scaleλisa continuous parameter,the exponentαθis related tothe critical exponentνof the correlation length asαθ=1ξ(θλ)=ξ(θ)αθwe obtain ξ∼|θ|−1|θ|ναµ)(26)where θλhas been scaled to ±1and ˜µλexpressed in terms of ˜µand θ.Differentiating this equation with respect to ˜µyields:<n >sing =(−θ)ν(d −αµ)∂F sing (X,Y )ν(d −αµ)singinto the ar-gument Y =˜µαµ(28)which defines the critical exponent 1αµin terms of the scaling exponent αµof the Yang-Lee zeros.Fig.5presents the scaling of the imaginary part of the µzeros for different values of the temperature.The linear regression slope of the logarithm of the imaginary part of the zeros plotted against the logarithm of the inverse lin-ear dimension of the simulation volume,increases when the temperature decreases from β=5to β=6.The re-sults of β=7.5correspond to αµ=1.3within the errors of the zeros as the simulation volume increases from 62to 82.As it is seen from Fig.3,we can trace zeros with similar real part (Re (µ1)≈0.7which is also consistentwith the critical value of the chemical potential given in Ref.[22])as the lattice size increases,which allows us to examine only the scaling of the imaginary part.Table 1presents the values of αµand 1αµδ0.5±0.0560.5±0.21.3±0.3∂µ,as a function ofthe chemical potential on an 82lattice.The location of the peaks of the susceptibility,rounded by the finite size effects,is in good agreement with the distribution of the real part of the Yang-Lee zeros in the complex µ-plane (see Fig.3)which is particularly evident in the β=7.5simulations (Fig.4(c)).The contribution of each zero to the susceptibility can be singled out by expressing the free energy as:F =2n x n yi =1(y −y i )(29)where y is the fugacity variable and y i is the correspond-ing zero of the partition function.The dotted lines on these plots correspond to the contribution of the nearby zeros while the full polynomial contribution is given by the solid lines.We see that the developing singularities are indeed governed by the zeros closest to the real axis.The sharpening of the singularity as the temperature de-creases is also in accordance with the dependence of the distribution of the zeros on the temperature.The singularities of the free energy and its derivative with respect to the chemical potential,can be related to the quasiparticle density of states.To do this we assume that single particle excitations accurately represent the spectrum of the system.The relationship between the average particle density and the density of states ρ(ω)is given by<n >=∞dω1dµ=ρsing (µ)∝1δ−1(32)and hence the rate of divergence of the density of states.As in the case of Lifshitz transitions the singularity of the particle number is rounded at finite temperature.However,for sufficiently low temperatures,the singular-ity of the density of states remains manifest in the free energy,the average particle density,and particle suscep-tibility [15].The regular part of the density of states does not contribute to the criticality,so we can concentrate on the singular part only.Consider a behaviour of the typedensity of states diverging as the−1ρsing(ω)∝(ω−µc)1δ.(33)with the valueδfor the particle number governed by thedivergence of the density of states(at low temperatures)in spite of thefinite-temperature rounding of the singu-larity itself.This rounding of the singularity is indeedreflected in the difference between the values ofαµatβ=5andβ=6.V.DISCUSSION AND OUTLOOKWe note that in ourfinite size scaling analysis we donot include logarithmic corrections.In particular,thesecorrections may prove significant when taking into ac-count the fact that we are dealing with a two-dimensionalsystem in which the pattern of the phase transition islikely to be of Kosterlitz-Thouless type[23].The loga-rithmic corrections to the scaling laws have been provenessential in a recent work of Kenna and Irving[24].In-clusion of these corrections would allow us to obtain thecritical exponents with higher accuracy.However,suchanalysis would require simulations on even larger lattices.The linearfits for the logarithmic scaling and the criti-cal exponents obtained,are to be viewed as approximatevalues reflecting the general behaviour of the Yang-Leezeros as the temperature and lattice size are varied.Al-though the bootstrap analysis provided us with accurateestimates of the statistical error on the values of the ex-pansion coefficients and the Yang-Lee zeros,the smallnumber of zeros obtained with sufficient accuracy doesnot allow us to claim higher precision for the critical ex-ponents on the basis of more elaboratefittings of the scal-ing behaviour.Thefinite-size effects may still be signifi-cant,especially as the simulation temperature decreases,thus affecting the scaling of the Yang-Lee zeros with thesystem rger lattice simulations will therefore berequired for an accurate evaluation of the critical expo-nent for the particle density and the density of states.Nevertheless,the onset of a singularity atfinite temper-ature,and its persistence as the lattice size increases,areevident.The estimate of the critical exponent for the diver-gence rate of the density of states of the quasiparticleexcitation spectrum is particularly relevant to the highT c superconductivity scenario based on the van Hove sin-gularities[25],[26],[27].It is emphasized in Ref.[25]thatthe logarithmic singularity of a two-dimensional electrongas can,due to electronic correlations,turn into a power-law divergence resulting in an extended saddle point atthe lattice momenta(π,0)and(0,π).In the case of the14.I.M.Barbour,A.J.Bell and E.G.Klepfish,Nucl.Phys.B389,285(1993).15.I.M.Lifshitz,JETP38,1569(1960).16.A.A.Abrikosov,Fundamentals of the Theory ofMetals North-Holland(1988).17.P.Hall,The Bootstrap and Edgeworth expansion,Springer(1992).18.S.R.White et al.,Phys.Rev.B40,506(1989).19.J.E.Hirsch,Phys.Rev.B28,4059(1983).20.M.Suzuki,Prog.Theor.Phys.56,1454(1976).21.A.Moreo, D.Scalapino and E.Dagotto,Phys.Rev.B43,11442(1991).22.N.Furukawa and M.Imada,J.Phys.Soc.Japan61,3331(1992).23.J.Kosterlitz and D.Thouless,J.Phys.C6,1181(1973);J.Kosterlitz,J.Phys.C7,1046(1974).24.R.Kenna and A.C.Irving,unpublished.25.K.Gofron et al.,Phys.Rev.Lett.73,3302(1994).26.D.M.Newns,P.C.Pattnaik and C.C.Tsuei,Phys.Rev.B43,3075(1991);D.M.Newns et al.,Phys.Rev.Lett.24,1264(1992);D.M.Newns et al.,Phys.Rev.Lett.73,1264(1994).27.E.Dagotto,A.Nazarenko and A.Moreo,Phys.Rev.Lett.74,310(1995).28.A.A.Abrikosov,J.C.Campuzano and K.Gofron,Physica(Amsterdam)214C,73(1993).29.D.S.Dessau et al.,Phys.Rev.Lett.71,2781(1993);D.M.King et al.,Phys.Rev.Lett.73,3298(1994);P.Aebi et al.,Phys.Rev.Lett.72,2757(1994).30.E.Dagotto, A.Nazarenko and M.Boninsegni,Phys.Rev.Lett.73,728(1994).31.N.Bulut,D.J.Scalapino and S.R.White,Phys.Rev.Lett.73,748(1994).32.S.R.White,Phys.Rev.B44,4670(1991);M.Veki´c and S.R.White,Phys.Rev.B47,1160 (1993).33.C.E.Creffield,E.G.Klepfish,E.R.Pike and SarbenSarkar,unpublished.Figure CaptionsFigure1Bootstrap distribution of normalized coefficients for ex-pansion(14)at different update chemical potentialµ0for an82lattice.The corresponding power of expansion is indicated in the topfigure.(a)β=5,(b)β=6,(c)β=7.5.Figure2Bootstrap distributions for the Yang-Lee zeros in the complexµplane closest to the real axis.(a)102lat-tice atβ=5,(b)102lattice atβ=6,(c)82lattice at β=7.5.Figure3Yang-Lee zeros in the complexµplane closest to the real axis.(a)β=5,(b)β=6,(c)β=7.5.The correspond-ing lattice size is shown in the top right-hand corner. Figure4Angular distribution of the Yang-Lee zeros in the com-plex fugacity plane Error bars are drawn where esti-mated.(a)β=5,(b)β=6,(c)β=7.5.Figure5Scaling of the imaginary part ofµ1(Re(µ1)≈=0.7)as a function of lattice size.αm u indicates the thefit of the logarithmic scaling.Figure6Electronic susceptibility as a function of chemical poten-tial for an82lattice.The solid line represents the con-tribution of all the2n x n y zeros and the dotted line the contribution of the six zeros nearest to the real-µaxis.(a)β=5,(b)β=6,(c)β=7.5.。

高三英语科学前沿单选题30题

高三英语科学前沿单选题30题

高三英语科学前沿单选题30题1.The discovery of a new planet is a major breakthrough in the field of_____.A.astronomyB.biologyC.chemistryD.physics答案:A。

本题考查名词词义辨析。

A 项“astronomy”天文学,发现新行星是天文学领域的重大突破;B 项“biology”生物学,与发现新行星无关;C 项“chemistry”化学,也不符合题意;D 项“physics”物理学,同样不涉及发现新行星。

2.The study of the human brain belongs to the field of_____.A.psychologyB.neuroscienceC.geologyD.mathematics答案:B。

A 项“psychology”心理学,主要研究心理现象;B 项“neuroscience”神经科学,研究人类大脑;C 项“geology”地质学,与大脑无关;D 项“mathematics”数学,也不涉及大脑研究。

3.The development of new materials is an important area in_____.A.engineeringB.literatureC.historyD.art答案:A。

A 项“engineering”工程学,涉及新材料的开发;B 项“literature”文学,不相关;C 项“history”历史,不符合;D 项“art”艺术,与新材料开发无关。

4.The research on climate change is mainly carried out in the field of_____.A.geographyB.economicsC.politicsD.music答案:A。

A 项“geography”地理学,气候变化的研究主要在地理学领域进行;B 项“economics”经济学,与气候变化研究的关系不大;C 项“politics”政治学,不是主要领域;D 项“music”音乐,完全不相关。

Kagome Spin Liquid戈薇的自旋液体

Kagome Spin Liquid戈薇的自旋液体
Triangular
Second Renormalization
Kagome
h (corr) 12 0.081
S 1S 2l1b ˆl2c ˆ
0.005 S1S2l1l2
- 0.039 S1 S2 ly1ly2
0.112 S1 S2
0.1 S 1S 2l 2b ˆ l 1c ˆ
n,n ~n
~n Z 1n P n n'n ~n' ~n' n
Step I: Divide lattice to disjoint blocks. Diagonalize H on each Block.
block excitations are the ''atoms'' (composite particles)
Truncate: M lowest states per block
• The triangular lattice flows to chiral symmetry breaking, probably the 3 sublattice Neel phase.
• Future: Investigations of the quantum phase transition in the effective Hamiltonian by following the RG flow.
Effective Bond Interactions
h( corr) 12

0.953
S 1S 2l1b ˆl2c ˆ

0.2111 S1S2l1l2
0.053 S1 S2 ly1ly2
0.1079 S1 S2

凝聚态物理英语

凝聚态物理英语

凝聚态物理英语全文共3篇示例,供读者参考篇1Condensed matter physics, also known as solid-state physics, is a branch of physics that deals with the physical properties of solids and liquids, such as conductors, semiconductors, and insulators. It is a highly multidisciplinary field that encompasses elements of quantum mechanics, statistical mechanics, and electromagnetism.One of the key concepts in condensed matter physics is the idea of collective behavior. In a solid or liquid, the individual atoms or molecules interact with each other in complex ways, leading to emergent phenomena that cannot be understood by studying the individual particles alone. For example, the behavior of electrons in a crystal lattice is governed by the collective interactions between them, leading to phenomena such as superconductivity and magnetism.Another important concept in condensed matter physics is symmetry breaking. In a system with particular symmetry, certain properties of the system are preserved under transformationssuch as rotations or translations. However, in a phase transition, the symmetry of the system is broken, leading to the emergence of new properties. For example, when a material undergoes a phase transition from a normal state to a superconducting state, the symmetry of the system is broken, leading to the emergence of perfect conductivity.Condensed matter physics is a highly active area of research, with ongoing investigation into phenomena such as topological insulators, quantum spin liquids, and high-temperature superconductors. These materials exhibit novel physical properties that could have profound implications for technology, such as faster computers and more efficient energy storage devices.In conclusion, condensed matter physics is a fascinating field that studies the physical properties of solids and liquids at the atomic and subatomic level. By understanding the complex interactions between particles in condensed matter systems, physicists can develop new materials with unique properties and advance our understanding of the fundamental laws of nature.篇2Condensed matter physics is a branch of physics that deals with the study of the physical properties of matter in its condensed phases, which include solids and liquids. This field of physics plays a crucial role in understanding the behavior of materials and their interactions at the atomic and subatomic level.One of the key concepts in condensed matter physics is the idea of symmetry breaking. Symmetry breaking refers to the process by which a system transitions from a symmetric state to a less symmetric state, leading to the emergence of new properties and phenomena. This phenomenon is responsible for the formation of structures such as crystals and magnets, which exhibit specific patterns and behaviors due to broken symmetries.Another important aspect of condensed matter physics is the study of phase transitions. Phase transitions occur when a material undergoes a change in its physical state, such as melting, freezing, or vaporization. Understanding the mechanisms and properties of phase transitions is crucial for developing new materials with unique properties and applications.One of the most exciting areas of research in condensed matter physics is the study of quantum materials. Quantummaterials display unique quantum mechanical properties, such as superconductivity and topological insulators, which have the potential to revolutionize technologies in fields such as electronics and energy storage.Overall, condensed matter physics is a diverse and dynamic field that continues to push the boundaries of our understanding of matter and its properties. By studying the behavior of materials at the atomic and subatomic level, physicists are able to develop new technologies and materials that have the potential to impact a wide range of industries. So yeah, Condensed matter physics is truly fascinating and holds immense potential for future discoveries.篇3Condensed matter physics is a branch of physics that deals with the physical properties of condensed phases of matter, such as solids and liquids. It is a highly interdisciplinary field that combines elements of physics, chemistry, materials science, and engineering to study the behavior of matter at the macroscopic level.One of the key goals of condensed matter physics is to understand the underlying principles that govern the behavior ofmaterials and to develop new materials with specific properties. This is important for a wide range of applications, from developing new electronic devices and sensors to designing new materials for energy storage and conversion.One of the key concepts in condensed matter physics is symmetry breaking. Symmetry breaking is a phenomenon in which the symmetry of a system is spontaneously broken, leading to the emergence of new properties and behaviors. For example, in a crystalline solid, the atoms are arranged in a regular, repeating pattern that exhibits translational symmetry. However, at low temperatures, the crystal may undergo a phase transition in which the symmetry is broken, leading to the emergence of new properties such as magnetic ordering or superconductivity.Another important concept in condensed matter physics is collective behavior. Condensed matter systems often exhibit complex collective behavior that emerges from the interactions between individual particles. For example, in a superconductor, the electrons pair up to form Cooper pairs, which then move through the material without resistance. This collective behavior is responsible for the unique properties of superconductors, such as zero electrical resistance and the expulsion of magnetic fields.Condensed matter physics also plays a critical role in advancing our understanding of quantum mechanics. Quantum mechanics is the branch of physics that describes the behavior of particles at the smallest scales, such as atoms and subatomic particles. In condensed matter systems, the behavior of electrons, atoms, and other particles is governed by the principles of quantum mechanics. Understanding how these principles manifest at the macroscopic level in condensed matter systems is essential for developing new materials with novel properties and applications.One of the key challenges in condensed matter physics is the complexity of the systems being studied. Condensed matter systems contain a large number of interacting particles, which can exhibit a wide range of behaviors and properties. This complexity makes it difficult to predict the behavior of condensed matter systems from first principles alone, and often requires the use of advanced theoretical and computational methods to model and simulate these systems.Despite these challenges, condensed matter physics has made significant contributions to our understanding of the physical world and has paved the way for numerous technological advances. From the discovery of new materialswith exotic properties to the development of new electronic devices and sensors, condensed matter physics continues to play a crucial role in shaping the future of science and technology.In conclusion, condensed matter physics is a vibrant and interdisciplinary field that studies the physical properties of condensed phases of matter. By exploring the principles of symmetry breaking, collective behavior, and quantum mechanics in condensed matter systems, researchers are able to develop new materials with novel properties and applications. As we continue to unlock the mysteries of condensed matter physics, we open up new possibilities for advancing science and technology in the 21st century.。

Magnon Bose condensation in symmetry breaking magnetic field

Magnon Bose condensation in symmetry breaking magnetic field

a r X i v :c o n d -m a t /0607711v 2 [c o n d -m a t .s t r -e l ] 1 S e p 2006Magnon Bose condensation in symmetry breaking magnetic field S.V.Maleyev,V.P.Plakhty,S.V.Grigoriev,A.I.Okorokov and A.V.Syromyatnikov Petersburg Nuclear Physics Institute,Gatchina,Leningrad District 188300,Russia E-mail:maleyev@.spb Abstract.Magnon Bose condensation (BC)in the symmetry breaking magnetic field is a result of unusual form of the Zeeman energy that has terms linear in the spin-wave operators and terms mixing excitations which momenta differ in the wave-vector of the magnetic structure.The following examples are considered:simple easy-plane tetragonal antiferromagnets (AFs),frustrated AF family R 2CuO 4,where R=Pr,Nd etc.,and cubic magnets with the Dzyaloshinskii-Moriya interaction (MnSi etc.).In all cases the BC is important when the magnetic field is comparable with the spin-wave gap.The theory is illustrated by existing experimental results.1.Introduction Magnon Bose condensation (BC)in magnetic field was intensively studied in spin singlet materials (see for example [1]and references therein).In this case magnons condens in the field just above the triplet gap.In this paper we consider magnon BC that appears in the symmetry breaking magnetic field.The theoretical discussion is illustrated by experimental observation of this BC in frustrated antiferromagnet (AF)Pr 2CuO 4and cubic helimagnets MnSi and FeGe.To clarify our idea we begin with consideration of conventional AFs.In textbooks two limiting cases are considered.First,the magnetic field is directed along the sublattices.In this case the system remains stable up to the critical field H C =∆,where ∆is the spin-wave gap.Then the first order transition occurs to the state in which the field is perpendicular to sublattices (spin-floptransition).Second,the field is perpendicular to initial staggered magnetization.The system remains stable but the spins are canted toward the field by the angle determined by sin ϑ=−H/(2SJ 0),where J 0=Jz ;J and z are the exchange interaction and the number of nearest neighbors,respectively.At H +2SJ 0the spin-flip transition occurs to the ferromagnetic state.To the best of our knowledge the first consideration of the symmetry breaking field was performed theoretically in [2]in connection with experimental study of the magnetic structure of the frustrated AF R 2CuO 4,where R=Pr,Nd,Sm and Eu [3,4].In these papers the non-collinear structure was observed using the neutron scattering in the field directed at angle of δ=450to the sublattices.It was found in[2]that in inclinedfield the Zeeman energy has unusual form with terms which are linear in the spin-wave operators and term mixing magnons which momenta differ in the AF vector k0.As a result the BC arises of the spin-waves with momenta equal to zero and±k0.Similar situation exists in cubic helimagnets MnSi etc.[5].If thefield is directed along the helix wave-vector k the plain helix transforms into conical structure and then the ferromagnetic spin state occurs at criticalfield H C.But if H⊥k the magnon condense with momenta zero,±k,±2k etc.This leads to the following observable phenomena:i)a transition to the state with k directed along thefield at H⊥∼H C1=∆√S/2(a l−a+l),l=1,2 and a l(a+l)are Bose operators.As a result the Zeeman energy has unusual formH Z=H a+q+k0a q+iϑN,i.e. these operators has to be considered as classical variables as in the Bogoliubov theory of the BC in dilute Bose gas.Due to thefirst term in(2)we must consider the operatorsa±k0and a+∓kas classical variables too.Minimizing the full Hamiltonian with respectto these variables we obtainE=(∆2sin22ϕ)/(16J0)−S2J0ϑ2−(H H⊥)2/[4J0(∆2(ϕ,H)],(3)where thefirst term is the energy of the square anisotropy.In cuprates with S=1/2ithas quantum origin and arises due to pseudodipolar in-plane interaction[9].The secondterm is the energy of the spin canting in perpendicularfield.The last term is the BCenergy and∆2(ϕ,H)=∆2cos4ϕ+H2⊥−H2 is the spin-wave gap in thefield[2].This contribution becomes important at H∼∆.The spin configuration is determined byd E/dϕ=0and equilibrium condition d2E/dϕ2≥0.This theory was verified by neutrons scattering[10,11].In diagonalfield H (1,1,0)the spin configuration in frustrated Pr2CuO4is governed by Eq.(3)and the intensityof the(1/2,1/2,−1)is given by I∼1+sin2ϕ[2].Neglecting the BC term we getsin2ϕ=−(H/H C)2,where H C=∆.As a result at H→H C we obtain I∼H C−H. But very close to H C the BC term becomes important and we have a crossover to I∼(H C−H)1/2.It is clearly seen infigure2.This crossover was observed in[10,11].3.Frustrated AFsIn frustrated R2CuO4AFs there are two copper spins in unit cell belonging to different CuO2planes(see inset infigure1).From symmetry considerations these spins do not interact in the exchange approximation.The orthogonal spin structure is a result of the interplane pseudodipolar interaction(PDI)[2,3]and the ground state energy is given by∆2E=on T we obtain H C≃7.8T andγC≃5.30that is in stronger disagreement wit the experiment.The experimentally obtained anglesαandγat T=18K andδ=9.50are shown infigure4[12].The transition to the collinear state withα∼−450andγC∼200 was observed.Again the non-BC theory can not explain the experimental data.For example it givesγC≃2.50.Explanation of all these experimental data using the BC theory will be given elsewhere.4.BC in helimagnetsIn helimagnets MnSi etc.Dzyaloshinskii-Moriya interaction(DMI)stabilizes the helical structure and the helix wave-vector has the form k=SD[ˆa׈b]/A,where D is the strength of the DMI,A is the spin-wave stiffness at momenta q≫k,ˆa andˆb are unit orthogonal vectors in the plane of the spin rotation.The classical energy depends on thefield component H along the vector k and the cone angle of the spin rotation is given by sinα=−H/H C,where H C=Ak2is the criticalfield of the transition into ferromagnetic state[5].However at H⊥≪H C rotation of the helix axis toward thefield direction and the second harmonic2k of the spin rotation were observed[6-8].Both phenomena are related to the magnon BC in perpendicularfield[5].The linear and mixing terms appear in the Zeeman energy in much the same way as it was discussed above:H Z=(H a−i H b)2the real form of the BC energy is not so simple.It is determined by nonlinear interactions but consideration of this problem is out of the scope of this paper.As a result the perpendicular susceptibility is proportional to1/(∆2−H2⊥/2)and 2k harmonic appears.The last was observed by neutron scattering[6-8].Intensities of corresponding Bragg satellites have the formI±∼[∆2/(∆2−H2⊥/2)]2[1∓(kP)]δ(q∓2k),(7) where P is the neutron polarization.If H⊥→∆√5.ConclusionsWe discuss a few examples of the magnon BC in symmetry breaking magneticfield.BC appears due to unusual terms in Zeeman energy.Obviously this phenomenon is very general and can be observed in other ordered magnetic systems.Effects related to the BC has to be more pronounced in thefield of order of the sin-wave gap.6.AcknowledgmentsThis work is partly supported by RFBR(Grants03-02-17340,06-02-16702and00-15-96814),Russian state programs”Quantum Macrophysics”,”Strongly Correlated electrons in Semiconductors,Metals,Superconductors and Magnetic Materials””Neutron Research of Solids”,Japan-Russian collaboration05-02-19889-JpPhysics-RFBR and Russian Science Support Foundation(A.V.S.).References1Crisan M,Tifrea I,Bodea D and Grosu I2005Phys.Rev.B721644142Petitgrand D,Maleyev S,Bourges P and Ivaniv A1999Phys.Rev.B5910793D.Petitgrand,Moudden A,Galez P and Boutrouille P1990J.Less-Common Metals164-165768 4ChattpodhayaT,Lynn J,Rosov N,Grigereit T,Barilo S and Zigunov D1994Phys.Rev.B49 99445Maleyev S2006Phys.Rev.B731744026Lebech B,Bernard J and Feltfoft1989J.Phys.:Condens.Matter161057Okorokov A,Grigoriev S,Chetverikov Yu,Maleyev S,Georgii R,B¨o ni P,Lamago D,EckerslebeH and Pranzas P2005Physica B3562598Grigoriev S,Maleyev S,Chetverikov Yu,Georgii R,B¨o ni P,Lamago D,Eckerlebe H and Pranzas P2005Phys.Rev B721344029Yildirim T,Harris A,Aharony A and Entin-Wohlman O1995Phys.Rev.B521023910Plakhty V,Maleyev S,Burlet P,Gavrilov S and Smirnov O1998Phys.Lett.A25020111Ivanov A and Petitgrand D2004J.Mag.Mag Materials272-27622012Plakhty V,Maleyev S,Gavrilov S,Bourdarot F,Pouget S and Barilo S2003Europhys.Lett.61 53413Ivanov A,Bourges P and Petitgrand D1999Physica B259-261879FiguresaFigure 1.Spin configuration in the field.Full and dashed arrows correspond to zero and nonzero field,respectively.Addition spin canting in H ⊥is shown by broken arrows.Inset:spin configuration in neighboring planes of frustrated AF.Figure 2.Log-Log plot of the (1/2,1/2,−1)Bragg intensity in diagonal field,h ∼(H C −H ).Figure3.Thefirst order transition in thefield directed along b axis.Calculated intensities for the spinflop configurations when spins are perpendicular to thefield (white arrows).Figure4.Field dependence of anglesαandγatδ=9.50.)10a H mT =)50b H mT =)150c H mT=Figure 5.Bragg reflections in the field along (1,1,0).a)Four strong spots corresponds to ±(1,1,1)and ±(1,1,−1)reflections.Weak spots are the double Bragg scattering.b)The 2k satellites appear.c)The helix vector is directed along the field.。

超分子及自组装超分子聚合物

超分子及自组装超分子聚合物
naturecommunications2014xrdx射线晶体衍射固态结构红外光谱和x射线光电子能谱分子结构sem和tem排列取向空间构象nmr分子结构和动力学特征超分子化学环境化学信息科学材料科学物理学生命科学分子信息化学信息储存分子识别分子水平结构特征修正传输处理水凝胶外壳涂料制备生物载药胶束佚名
1894年荷兰 科学家Emil Fischer提出 了我们熟知 的“锁钥模 型”
1967年杜邦 公司的C.J. Pederson首 次报道了二 苯并18-冠-6
1987 年 J. M. Lehn 教授首 先提出来的,关于这一概 念的解释是“基于共价键 存在着分子化学领域,基 于分子组装体和分子间键 存在着超分子化学
Shen Z, Jiang Y, Wang T, et al. Symmetry Breaking in the Supramolecular Gels of an Achiral Gelator Exclusively Driven by π–π Stacking*J+. Journal of the American Chemical Society, 2015, 137(51): 16109-16115.
超 分 子 配 合 物
Toshimitsu F, Nakashima N. Semiconducting single-walled carbon nanotubes sorting with a removable solubilizer based on dynamic supramolecular coordination chemistry[J]. Nature communications, 2014, 5.
π−π stacking
可生物降解 的二硫键 喜树碱

物理作文押题英语模板

物理作文押题英语模板

物理作文押题英语模板英文回答:Introduction。

Physics is the fundamental science that studies the basic laws of nature and their applications to various phenomena. It plays a pivotal role in understanding the universe, from the smallest subatomic particles to the largest galaxies. As we approach the frontiers ofscientific discovery, it is essential to explore the future directions of physics research and identify emerging trends that will shape the field in the years to come.Emerging Trends in Physics。

1. Quantum Computing。

Quantum computing harnesses the principles of quantum mechanics to perform complex calculations that areintractable for classical computers. This technology has the potential to revolutionize fields such as cryptography, drug discovery, and materials science.2. Artificial Intelligence (AI)。

AI is rapidly transforming various industries,including physics. Machine learning algorithms can analyze vast amounts of data, identify patterns, and make predictions, aiding in experimental design and data analysis.3. Gravitational Waves。

The Monte Carlo method in quantum field theory

The Monte Carlo method in quantum field theory
1
arXiv:hep-lat/0702020v1 20 Feb 2007
THE MONTE CARLO METHOD IN QUANTUM FIELD THEORY
COLIN MORNINGSTAR Department of Physics, Carnegie Mellon University, Pittsburgh, PA 15213, USA E-mail: colin morningstar@ This series of six lectures is an introduction to using the Monte Carlo method to carry out nonperturbative studies in quantum field theories. Path integrals in quantum field theory are reviewed, and their evaluation by the Monte Carlo method with Markov-chain based importance sampling is presented. Properties of Markov chains are discussed in detail and several proofs are presented, culminating in the fundamental limit theorem for irreducible Markov chains. The example of a real scalar field theory is used to illustrate the MetropolisHastings method and to demonstrate the effectiveness of an action-preserving (microcanonical) local updating algorithm in reducing autocorrelations. The goal of these lectures is to provide the beginner with the basic skills needed to start carrying out Monte Carlo studies in quantum field theories, as well as to present the underlying theoretical foundations of the method. Keywords : Monte Carlo, Markov chains, Lattice QCD.

英语专业四级考试——50组近义词辨析

英语专业四级考试——50组近义词辨析

英语专业四级考试——50组近义词辨析在学习英语词汇中,有时同义词的辨析是很不容易的,我们一般从三方面进行区分,即:语法、语义和文体。

语法主要是词性、搭配、句式等的区分;语义主要是词义的本义、引申义、比喻义和内涵和外延等的区分;文体主要是正式和非正式、褒义和贬义等的区分。

1.路way: Wherever there is room for an object to proceed, there is a way.road: A road is a prepared way for traveling with horses or vehicles.path: A way suitable to be traveled only by foot passengers or by animals.route: A route is a line of travel, and may be over many roads.street: A street is in some centre of habitation, as a city town or village, when it passes between houses of dwellings.avenue: A avenue is a long, broad and imposing(庄严) or principal street.2.时代(期) (时期)period: It indicates any passage of time, great or small. /an extent of time of any length. ( 时代)time(s): It refers to a period in history. in ancient times/ in Victoria time ( 新时代) epoch: It indicates a long period of time marked by events or development of a particular kind.The first flight into space marked a new epoch in the history of mankind. (纪元)era: It refers to a very long period of time marked by a particular feature in a great new era of world revolution ( 时期)age: It shows a particular /a fairly definite period in history. the Bronze Age, Iron Age3.战斗(打仗)fight: It is a bodily struggle ( 奋斗斗争)struggle: An effort of any kind to overcome difficulty. ( 战斗)battle: A fight between armed forces. ( 战役)campaign: A series of related military operations in a war. ( 战争)war: A period of fight between countries or states when weapons are used and many people are killed.( 对抗)combat: A fight, conflict, controversy.4.牧师(教士牧师) #priest: A person, esp. a man specially trained for various religious duties and ceremonies, in the Christian church, esp. in the Roman Catholic church ( 牧师)minister: A member of clergy, esp. Protestant churches. ( 牧师)clergy(pl): The officially appointed leader of the religious activities of a particular church or temple.clergyman: clergymen(pl) a member of clergy. ( 牧师)pastor: A Christian religious leader in charge of a church and its members, esp. in a Protestant church. ( 教区牧师)vicar: A priest in charge of an area(parish) in the church of England.father: A little of respect for a priest, esp. in the Roman Catholic.5.服装clothing(collect): (fml) General term of clothes.clothes(no single): Coverings of the body such as coats, dresses, suits, shoes, hats.garment(fl): A suit of clothes used by actors./a single article of clothing.costume: 1) The fashion of dress peculiar to a people, nation, class, period, etc.2) A dress worn by actors in a play. uniform: worn by all members of the community.dress: 1) A kind of outer garment worn by women ( 连衣裙).2) worn on special occasions (礼服) evening dress/ morning dresssuit: A set of outer clothes to be worn together. evening suit/swimming suitcoat: A garment with sleeves worn on top of other clothes from rain, heat, etc.overcoat: A warn coat worn in the street.6.哭cry: The most general one.(哭泣) weep: To let flow tears.(抽泣抽嗒) sob: To weep or sigh with short quick breaths.(哭天抹泪涕泪交流) snivel: To sniffle and cry in a irritating manner.(哭嚎又哭又闹) blubber: To cry loudly noisily.(发出低声报怨声) whine: To make a low complaining cry.(嚎哭) bawl: To utter loud cries (always in bad sense).(痛哭) wail: To cry aloud from pain or sorrow.(呻吟) moan: To make a low, miserable sound in pain or sorrow.(呻吟) grown: To make a low sound of pain, unhappiness or disapproval(哀悼) mourn: To feel or show sadness or sorrow for someone who has died.(哀悼) lament: To express great sorrow or regret.7.美丽漂亮good-looking: Having an attractive appearance in a strong, healthy way used for men and women not things.beautiful: ( a woman or a thing) Suggesting symmetry of features or perfection of proportion, elegance and mobility. beautiful flowers, a beautiful girl/voice/city/face beautiful weather.handsome: Of attractive appearance applies to men. a handsomefellow/actor/horse/buildings/young man.pretty: (a girl, or a small thing) Suggesting liveliness and sweetness, pleasing or nice to look at. a pretty little woman/garden, a pretty girl/ picture/piece of music,lovely: (something) So beautiful that it makes you feel good to look at it or even to think about it. The garden looks lovely.fair: Beautiful( of woman in poet) light in color esp., skin hair.gorgeous: (persons or things) (inf) Extremely beautiful or handsome.8.拉拖pull: The most general one.draw: It implies a smoother, steadier motion and generally a lighter force than pull.drag: It usually refers to horizontal motion or motion up an incline (slope) and it suggests laborious efforts over rough ground or against friction, resistance or gravity. The escaped prisoner was dragged out of his hiding place.haul: It implies continuous pulling or dragging of heavy or bulky objects. The fisherman is hauling a net.tug: It applies to hard often sudden violent effort to pull. He tugged at my sleeve to ask directions.jerk: To pull suddenly. He jerked out the knife that was stuck in the wound.tow: To pull by a rope or chain. We towed the car to the nearest garage.wrench: To pull hard with a twisting or turning movement.9.旋转turn: The most general one.( 自转) spin:To turn quickly around a central point. It emphasizes the continuity of the action, and usually the narrow extent of the circular motion. The wheel is spinning on its axis.( 急转) whirl:To round very fast. It implies the lock of conscious control.(转动) rotate: To turn round a fixed point with a circular movement. The earth rotates once every 24 hours.(绕转) revolve:To turn or move in a circle around a central point. It indicates circular or elliptical (椭圆) movement. The planets revolve around the sun.10.生气气愤anger: The most general one.(易怒) be cross:Feeling easy to get angry.(愤慨) indignation:(fml) Anger. It stresses righteous anger at what one considers unfair, mean or shameful.We expressed our indignation at the ruthless exploitation.(愤怒) wrath:Very treat anger. (literary) It suggests a desire on intent to revenge or punish.(狂怒) rage: Wild, violent anger. It suggests loss of self- control from violence of emotion. in a rage /to fall into a rage.(暴怒) fury: Violent, extreme and destructive anger. She flew into a fury.11.错误(误会) mistake: A wrong thought, act. It implies carelessness. Anyone can make a mistake.(过错弱点) fault: A bad point, but not of a serious moral kind. It refers to behavior and character. His only fault is that he lacks ambition.find fault with sb / at faultshortcoming: weakness, failing ; It refers to failures or deficiencies in things as well as people.In spite of all her shortcomings I still think she's one of the best teachers in the school.(疏忽) error: A mistake (formal sometimes literary) It implies deviation from a standard or modelThe accident was caused by human error.(缺点毛病) defect: sth lacking or imperfect. It refers to quality.The radio was returned because of a defect.(失误过失) blunder: A very stupid or unnecessary mistake. It implies ignorance.This is the fatal blunder of his life.12.图画picture: The most general one.(彩图) painting: pictures with color.(绘画图画) drawing: A picture made with a pen, pencil and crayon. Sketch, diagrams and graphs are all drawings.(草图) sketch: A rough not detailed drawing.(图解图表) diagram: A drawing, figure that shows the arrangement of something.(曲线图) graph:A diagram in which a straight line, curved, or zigzag line shows how two sets of numbers or measurements are related.(插图) illustration: A picture to go with words of a book.(图样草图) draft: The first rough written form of anything.(平面图) plan:A line drawing of a building as it might been seen from above.(主视图) elevation:A flat upright side of a building.(海图) chart: A map esp. a detailed map of a sea area.13.特别(专门的,与众不同的) special:Different in some way from what is common, ordinary, or usual. It stresses having a quality, character, identity, or use of its own. The tube contains special gases.(特别的) especial:(fml) To an usually great degree, exceptional; It emphasizes the importance of the things or thepersons mentioned; This is a matter of especial importance. (个别的) particular:Relating or belonging to only one thing or person. It stresses the distinctness of something as anindividual which is worth notice. In that particular case, the rule doesn't hold.(适用)(特种的) specific:Detailed and exact, clear in meaning and explanation, fixed, determined.(used in scientificarticles) It implies a quality or character distinguishing a kind or a species.He gave me a very specific instruction. There is a specific tool for each job.(独特的) peculiar: Strange or perhaps unpleasant. It implies strangeness. He has a peculiar way of speaking.14.取消消灭(取消解除) cancel:To give up, to declare something is to be effective. He has cancelled his leave of absence.(消假)(废除废止) abolish:To do away with. It refers to practices, social institutions. Bad customs should be abolished.(消灭排除) eliminate:To get rid of. We should eliminate the false and retain the true. (撤消废除) repeal: To bring to an end of the effect of a law or an order. Some laws should be repealed.(根除消灭) exterminate:To destroy completely and wholly. Colonialism must be exterminated.15.破碎break: The most general one.(压碎压破) crush: To press together violently as to break, to destroy its shape by squeezing it. It suggests the effect of great external pressure. The tree fell on top of the car and crushed it.(打碎) smash: To break thoroughly to pieces with a crushing sound. She dropped the plate and smashed it.(打裂) crack:To break without separation of parts. It suggests the breaking out across a surface. He cracked the window by leaning against it.(破裂) burst:To break open by pressure from within. The fireworks burst while they were in the air.(砸碎破碎) shatter: To break into pieces. It suggests the breaking up of a thin surface. The glass was shattered to pieces.(撞坏) crash: To refer to the vehicle which hits something and is badly damaged.16.环境形势(环境形势) conditions:The location and other factors likely to affect it. It suggests something that has stayed the same for some time and which affects daily life such as food, work, and houses. We are now studying the economic conditions in the developing countries. (形势) situation: A position or state at a particular time, set of conditions, facts, and events having an effect on a person, society, etc. It suggests more general matters such as government planning and finance. The political situation in these countries are always changing.(环境周围外界) environment: The circumstances, things and conditions that influence you. It refers to spirit aspect, physical aspect and material aspect. We must try to beautify our environment.(形势情况) circumstance(s): A situation or event around us, a certain kind of atmosphere, the conditions that affect what happens. in (under) the circumstances(环境周围事物) surrounding(s): The area and environment around a place or person. It indicates a very narrow condition, "physically" sometimes reflects spiritual aspect. They lived in hostile surroundings.17.著名的well-known: (infl)famous: The most general one. widely known or honored.(杰出的知名的) distinguished: Great, outstanding marked by excellent quality or deserved fame, used especially of people who are famous for serious work in science, the arts etc. He was a distinguished writer.(驰名的) celebrated: Famous, (substitute for renowned) It refers objectively to sb or something that has been give acclaim or honoured with awards or prizes. She was a celebrated actress.renowned: Highly honored and famous for something good. often refers to places or things, also It suggests something that has become legendary or is no longer available for an objective evaluation. Edison was renowned for his inventions.noted: Well-known and admired It often describes a more intellectual kind of effort and accomplishment indicating an authority or expert or their theories. Maybe it is not widely known to the general public. He was a very noted expert.(臭名昭著) notorious:Famous for something bad. He is notorious for his crimes.18.强盗thief: The most general one.(强盗) robber:It suggests a direct confrontation in which the owner is forced to give up his valuables.(行凶强劫) mugger: A person who attacks and robs people in a street or in a lift. burglar: A person who breaks into a house at night to steal something.(歹徒暴徒) gangster: A member of a group of criminals, esp. those who are armed and use guns to threaten.(匪徒) bandit: an armed robber. It suggests an organized group in a rural setting.(土匪) brigand: A robber who lives by robbing travelers in the country.(海盗) pirate: A person who robs on the sea.19.摇动,颤动shake: The most general one. to move up and down or back and forth. It refers to persons or things.(发抖) quiver:To tremble a little. It suggests a rapid but invisible vibration. His lips quivered with emotion.(颤抖) tremble: To shake uncontrollably and slightly as from fear, cold, excitement etc. It implies uneasiness and nervousness. Her voice trembled as she began to sing.(瞬间发抖) shiver: To tremble from fear or cold. It suggests a slight and rapid movement. He stood shivering in the snow.(极度颤动) quake: to shake or tremble violently. It suggests a more violent and sudden change. He quaked with excitement. An explosion cam make the ground quake.(抽筋般颤动) shudder:To shake uncontrollably for a movement. It suggests a more intense shaking. She shuddered at the sight of a snake.20.说话谈话(说话) speak: To use your voice to say words.(说) say:To speak words.(发出声音) utter: To make sound and say words.drawl: To speak in a slow, prolonged manner.mutter: To express displeasure with compressed lips.rave: To talk in an angry, uncontrolled way.gabble: To talk rapidly, making inarticulate sounds.(谈论) remark:To mention it or comment on it.(陈述) state:To say, express or put into words, esp. formally. He stated his view.(讲述) narrate: To tell formally in writing or speech or describe something in order with intonation. He narrated his adventure in the forest.(详述) relate:To tell formally in details, to give an account of. He related his experiences. (讲演) address:To say in speech or writing to a person or group.tell: To let people know about something.talk: To say things to someone.converse: To talk formally. The scholars are conversing with each other on linguistics. chat: To talk in a friendly, familiar, informal manner. The two friends sat in a corner and chatted.chatter: To talk continuously rapidly about small things. The schoolgirls went along chattering.whisper: To talk in a low voice. She whispered me not to talk so loudly.murmur: To make a soft sound, esp. to speak or say in a quiet voice. He often murmurs to himself.(闲谈) gossip: To talk about the details of other people's actions and private lives which may not correct or proper. That woman is very fond of gossiping about others. stammer: To speak with pauses and repeated sounds because of excitement, embarrassment. stutter: To speak with pauses and repeated sounds because of inherent speech defect.21.事情,事件(事) thing:An event, a fact, a subject. He talked of many interesting things.(事情) matter:Seth that you have to deal with, something to be discussed, thought over. There are several matters to be dealt with at the meeting.(事务责任) business:A special duty, something that has to be done. Public business is every one's business.(事务) affair: An event or set of connected events. (pl) private and personal life. I have many affairs to look after.(事件) event:An important happening. Events such as birthdays and anniversaries are often celebrated. Do you know the chief events of 1986.incident: Not as important as an event. Incidents seldom are celebrated. Sometimes an event becomes an incident after many years have passed.(偶然事件) happening:An occurrence, and sometimes an unusual one. There have been strange happenings here lately.(偶发事件) occurrence: An incident that is usually unexpected and has not been planned ahead of time. Flood is practically an annual occurrence in this district.22.承认admit: To agree to the truth of, usu, something bad. It suggests reluctance or possible objection. He admitted his crime/stealing.(自白供认) confess:To admit guilt as to a crime or as to a shortcoming, in the sense of making known to others one's own error or wrong doing. He confessed his fault/doing something wrong.acknowledge: to agree the truth of, recognize the fact or existence of what have said or done, good or bad. It emphasizes openly in a embarrassing or awkward and usually not voluntary way. I acknowledged my signature/mistakes/errors/having been defeated.grant: To admit or to agree something is true. I granted his request/his honesty. take sth/sb for granted.concede: To admit as true, just or proper often unwillingly because of overwhelming evidence. I conceded you that point, but I still think you are wrong.recognize: To accept or acknowledge it. It refers to something about law and diplomacy. The new regime was recognized by China.23.走路walk: The most general one.stride: To walk with long steps. He strode through the station a few minutes before the train left.(高视阔步) stalk: To walk stiffly, slowly, and proudly with long steps.trot: To jog, move quickly, usu refers to horses.(蹒跚而行) waddle: To walk from side to side with short steps like a duck. The fat man waddled out of the room.(蹒跚) stagger:To walk unsteadily, slide and drag the feet almost falling at each step, usually because of illness, injury or drink. After drinking too much, he staggered in the street.(摇摆蹒跚) totter:To walk unsteadily showing great weakness often used of very young children learning to walk. The child tottered before his parents.(拖着脚走) shuffle: To move without lifting the feet clear of the floor as if wearing slippers. The old man shuffled along the road.(趾高气扬地走) strut: To walk in a proud strong way, esp. with the chest out and trying to look important.(慢行) amble:To walk at an easy gentle rate. It stresses a leisurely but regular movement. (闲逛) stroll:To walk, esp. slowly, for pleasure. It emphasizes a slower movement, more wandering and aimless with suggestions of many starts and pauses. They are strolling through this park.saunter: A little more formal than stroll.(漫步徘徊) wander:To move about without a fixed course, aim, or purpose. He was wandering about/down/through/up and down the street.(漫游) roam:To wander with as very clear aim. It suggests a more serious purpose behind the irregular of circular movement in complete forgetfulness of time. The lovers roamed around/through the fields.(跋涉) trudge: To walk heavily and wearily with effort as when one (plod) is tired. The hunter was trudging through the deep snow.(重步行走) tramp:To walk with firm heavy steps. Who has been tramping all over the carpet in muddy shoes.(扭扭捏捏地走) mince: To walk with little short steps in an affected manner. It was a funny sight to see her mince along.slouch: To walk in a loose, ungainly ( 不雅观) way.hustle: To walk in a busy, active way.24.跳jump: The most general one. to throw oneself into the air.(跳起) leap: (literary) To spring through the air, often landing in a different place. The boy leaped over the brook without difficulty.(跳跃) spring: To leap suddenly and quickly. He sprang to his feet at the sudden noise. (跳着跑) bound:To spring lightly along. It suggests high spirits and excitement. His dog bounded to meet me.(轻快地跑) skip:To move in a slight dancing way, as with quick steps and jumps. The little girl skipped at her mother's side.hop: To jump on one leg. The boy had hurt his leg and had to hop along.vault: To leap over something using the hands or a pole. You can vault a fence by putting your hands on it and swinging yourself over.hurdle: To jump over some thing while running. The horse hurdled the fence and ran into the woods.25.特点特征quality: The most general one.(特点) characteristic: Quality typical of a particular person and thing, a special and easily recognized quality of sb/sth. It has many scientific or technical uses. It implies neutral description in referring to any aspect of something without evaluating its relative importance to the whole. A useful characteristic of the cat is its ability to catch and kill mice. (特征) character: The combination of qualities which make a particular person, thing, place, etc. A tendency not to show emotions is supposed to be part of the British national character.(性质) nature:The qualities make someone or something different from others. It indicates the widest range of traits, including emotional, mental and physical qualities. It is only human nature to like money.(特征) attribute: A quality belonging to or forming part of the mature of a person or thing. The word is positive rather than negative. Darkness is an attribute of night.(特性) peculiarity:The quality of being peculiar, strangeness, unusualness. It shows an unpleasant attribute that is quite noticeable. One of his peculiarities is that his two eyes are not the same size.(特色) feature:A typical and noticeable part or quality. It suggests something positive and specifically. It refers to physical appearance. A lake is an important feature in this area. (品质特性) trait:A particular quality of sb/sth. It refers to more abstract attributes. Honesty and diligence are the chief traits of his character.(个性) personality: The whole nature or character of a particular person. It refers to the whole indefinable emotional coloration that a specific person gives off. He has a strong personality.26.增加increase: To make or become larger in amount or number. it refers to quantity or intensity as well as size. The population of this county has increased.add: To put together with something else so as to increase the number size, importance. He added some wood to increase the fire.(扩大) enlarge: To grown larger or wider. I want to enlarge this photograph/house.(放大) magnify:To make something appear larger than in reality, esp. by means of a lens. You have magnified the peril.(扩充) amplify: To make large or fuller, esp. give fuller information, more details etc. to amplify a radio signal/sound.augment: (fml) To become larger or greater. It emphasizes the action of addition. He augmented his income by writing some short stories.(扩展扩张) expand: To increase in range scope or volume as well as in size. Iron expands when it is heated.(加长) extend: To make longer in space or time, to extend a railway. Can't you extend your visit for a few days.27.笑(微笑) smile:The corners of your mouth move outwards and slightly upwards. He smiles his consent./with satisfaction.(大笑) laugh:To make a noise to show one's amusement and happiness. You can laugh at a joke or at an amusing sight. You can laugh at someone without being amused. They all laughed loudly.(露齿而笑) grin: To smile with the teeth. The boy grinned from ear to ear when I gave him a sweet.(暗笑含笑) chuckle: To laugh quietly. I could hear him chuckling to himself as he read that funny article.(咯咯笑) giggle: To laugh repeatedly foolishly and uncontrollably, esp. by girls. I heard them giggle when I passed by the girls.(窃笑暗笑) snicker: To laugh in a disrespectful more or less secret way. On hearing his absurd opinion, I went snickering.(假笑痴笑) simper:To smile in a silly unnatural way. When I told him the thing, he simply simpered.(得意的笑) smirk: To smile in a false or too satisfied way. He smirked at everyone that passed.(窃笑) titter:To laugh very quietly from nervousness or badly controlled amusement. The girls tittered when they heard this.(狂笑) guffaw: To laugh loudly and rudely. All the people guffawed at his silly words. (哄笑) roar:To laugh long and loudly. They roared after they heard the joke.(欢笑) chortle: To give a laugh of pleasure or satisfaction. He chortled with delight when I told him the news.(笑骂) taunt:To try to make sb angry, or upset by making unkind remarks, laughing at faults or failures. They taunted her with her inability to swim.(嘲笑嘲弄) ridicule: To laugh unkindly at or to make unkind fun of. They all ridiculed the idea.(讥笑) deride: To laugh at or make fun of as of no value. /to mock at someone with contempt They all derided his foolishness.(嘲弄) mock:To laugh at sb(sth) when it is wrong to do so, esp. by copying in a funny or contemptuous way. The students mocked the seriousness of his expression.twit: (infl) To make fun of sb because of behavior, a mistake, a fault, etc. He twitted her with her timidity.(嘲笑轻蔑地笑) scoff: To laugh at, to speak or act disrespectfully. /To speak in scornful mocking way. It was a great invention but at first many people scoffed at it.(戏弄) chaff: (infl) To make fun of sb in a good-humored way. He chaffed the man about his mistakes in speaking English.(讥笑) jeer: To laugh rudely at /to insult sb in a loud, unpleasant way. They always jeer at the priests.gibe(jibe): To laugh at with the intention of hurting the feeling with sarcastic remarks. Don't gibe at her behavior until you know the reason for it.(讥笑冷笑) sneer:To express proud dislike by a kind of usu, one- side smile or to show scorn or contempt by looks. She sneered at the furniture in his neighbor's home.joke: To make fun of. You mustn't joke with him about religion.(取笑) jest: To act or speak playful, not seriously. Don't jest about serious things.(戏弄) banter: To speak, or act playfully or jokingly. We bantered him on the subject of marriage.(轻视) scorn: To look down upon.28.疯mad: Showing that one has amanita illness which often causes them to behave in strange way.crazy: (infl) Very strange or foolish.psychotic: The most precise one. used by psychiatrists.insane: Not sound in mind. Used in scientific articles.lunatic: (old derog) wildly foolish.demented: It indicates sb's mentality has degenerated from a precious level.maniac: (n) A mad person who is violent and dangerous.29.味道smell: The most general one. It refers to something pleasant or unpleasant.odo(u)r: (fml) More used in scientific articles.fragrance: A sweet or pleasant smell. It refers to flowers and stresses a delicate smell from plants. Those roses have a delightful fragrance.scent: A smell esp. left by an animals, an pleasant smell. Our dog lost the fox's scent. perfume: A sweet or pleasant smell. It refers to either natural smell or a man-made smell and stresses a strong and rich smell compared with fragrancearoma: A strong usu pleasant smell, often a spicy smell.flavor: The particular quality of tasting good or pleasantly strong. The bread hasn't much flavor.savor: The smell of food by the processes of cooking. The meat had cooked too long and lost its savor.stink: A strong unpleasant smell. the stink of sweaty feet.stench: A very strong unpleasant smell.30.怕fear: The feeling that one has when danger is near.(可怕) dread: A great fear esp. of some harm to come. It suggests fear of facing whatever is coming. Usually dread also means loss of courage. Illness is the great dread of his life. (畏惧) fright:The feeling or experience of fear. sudden great fear. I nearly died of fright at the sight of escaped lion.(恐慌) alarm:Sudden fear and anxiety as caused by the possibility of danger and excitement caused by fear of danger. The news caused great alarm.(恐惧) terror:Extreme and intense fear. The people ran from the enemy in terror.(恐怖战栗) horror:A feeling of great shock, fear and dislike. I cried out in horror as I saw the man killed.(惊恐万状) panic:Sudden uncontrollable quickly-spreading fear or terror, which results in unreasonable and frantic activity. When I realized the situation I got into a panic.(敬畏) awe: A feeling respect mixed with fear and wonder. He always stands in awe of his father.31.闪光shine: The most general one.(闪耀) glitter: To shine brightly with flashing points of light. All that glitters is not gold. (发火花) sparkle:To shine in small flashes. It suggests uneven, bright flashes reflected from light-catching objects. We can see a diamond sparkling in the sunlight.(闪光) flash: To give out a sudden and monetary bright ray of light/ To shine suddenly for a moment.(闪耀) glisten: To shine from or as if from a wet surface. His hair glistened with oil. The wet road glistened.(闪烁) gleam: To send out a bright light moderately, mildly not violently. A cat's eye gleamed in the dark. The lantern gleamed.(冒火花) spark: To send out small bits of fire. He was so angry that his eyes sparked furiously.。

Peskin量子场论习题解答(第三学期)

Peskin量子场论习题解答(第三学期)

Physics 332–Problem Set #2(due Wednesday,April 26)1.Peskin and Schroeder,Problem 11.1.2.Peskin and Schroeder,Problem 11.2.3.Peskin and Schroeder,Problem 11.3.1Physics 332–Problem Set #3(due Wednesday,May 3)1.Peskin and Schroeder,Problem 12.1.2.Peskin and Schroeder,Problem 12.2.You should show that,with this βfunction,the mass m ψof the ψfield satisfies the Callan-Symanzik equation M ∂∂M +∂g m 12(4π)4+(4π)4+Physics 332–Problem Set #4(due Wednesday,May 10)1.Peskin and Schroeder,Problem 12.3.2.Peskin and Schroeder,Problem 13.1.1Physics 332–Problem Set #5(due Wednesday,May 17)1.Consider scalar electrodynamics:L =−14(F 6(φ48π224π2(5λ6λ(ϕ 2.Apply the methods of this problem to the Glashow-Salam-Weinberg model of weak interactions.(a)Compute the effective potential for the Higgs field to 1-loop order,ignoring all effects of quark masses but including the contributions of gauge fields.(b)Show that the theory has a first-order phase transition as a function of the renor-malized Higgs mass parameter μ2.(c)Show that this result implies a lower bound on the physical mass of the Higgs boson (the ‘Linde-Weinberg bound’).Compute the bound to leading order in coupling constants.(d)Now add in the contribution of the top quark.Show that,when the top quark mass is sufficiently heavy,the symmetry-breaking effect found in part (b)goes away.However,another pathology develops,in which,when m t is sufficiently large,the effective potential becomes negative at very large field values and causes an instability of the model.Estimate the value of the top quark mass,as a function of the Higgs boson and W boson masses,at which this instability takes place.2Physics 332–Problem Set #6(due Wednesday,May 24)1.Peskin and Schroeder,Problem 17.1.2.In class,I sketched the derivation of the βfunction of a non-Abeliangauge theory from the renormalization counterterms δ1,δ2,and δ3.Work through this calculation in full e the Feynman-‘t Hooft gauge.3.Peskin and Schroeder,Problem 16.3.Please note:This is a long calculation.The solution set for this problem set is 50pages long,of which 35pages are devoted to this problem.I do assure you that you will learn a considerable amount about how to calculation in gauge theories by doing this problem to the end.(Of course,it might be true that these are things that you never wanted to know ...)1。

理想的爱人英语作文

理想的爱人英语作文

理想的爱人英语作文英文回答:In the realm of love, the quest for an ideal partner is an elusive endeavor, yet one that has captivated hearts and minds throughout the ages. While there is no universally accepted definition of an ideal lover, certain qualities emerge as common threads in the tapestry of romantic aspirations.In the physical realm, many seek a partner who embodies beauty and grace. However, true beauty extends beyond superficial attributes to encompass the inner radiance that emanates from a kind heart and a vibrant spirit. A person's eyes, often regarded as the windows to their soul, hold the promise of a deep and meaningful connection. Symmetry and balance in facial features are also consideredaesthetically pleasing, but it is the imperfections that humanize us and make us uniquely charming.Intellect and wit are highly prized qualities in an ideal lover. A sharp mind and a thirst for knowledge are not only attractive but also provide endless opportunities for stimulating conversations and shared experiences. The ability to engage in thoughtful debates and share passionate discussions about life's mysteries, current events, and the meaning of it all is paramount. Moreover, a sense of humor is essential for lightening the mood, breaking the ice, and creating a joyful ambiance.Emotional intelligence and empathy are crucial virtues that foster a profound bond between lovers. The capacity to understand and reciprocate each other's feelings, offer support during challenging times, and celebrate triumphs together is indispensable. A genuine and caring nature, devoid of judgment and pretension, creates a safe and nurturing space where both partners can flourish and grow emotionally.Trust and loyalty are the cornerstones of a healthy and fulfilling relationship. To feel secure in the knowledge that one's partner is faithful, reliable, and committed isessential for peace of mind and happiness. Trust andloyalty go hand in hand with open and honest communication, which forms the foundation of a strong and lasting bond.Beyond these core qualities, compatibility plays a significant role in determining the ideal lover. Shared values, beliefs, and interests create a common ground upon which a relationship can thrive. A sense of adventure and a zest for life are also highly desirable, as they provide opportunities for creating lasting memories and experiencing new things together.Lastly, it is important to acknowledge that the ideal lover is not a static entity but an evolving concept that changes with our own experiences and perspectives. As we grow and mature, our definition of the ideal lover may also evolve. It is a dynamic and ever-changing journey that should be embraced with openness and a willingness to learn and grow.中文回答:理想的爱人是一个充满魅力、呵护备至、令人心生向往的人。

数学很重要英语作文

数学很重要英语作文

数学很重要英语作文Mathematics is an essential subject that plays a crucial role in our daily lives. It is not only important for academic and professional success, but also for our overall cognitive development. In this essay, we will explore the significance of mathematics and its impact on our lives.First and foremost, mathematics is fundamental in shaping our logical thinking and problem-solving skills. It provides us with the ability to analyze and solve complex problems by breaking them down into smaller, more manageable parts. This skill is not only valuable in academic settings, but also in real-life situations, such as budgeting, planning, and decision-making. For example, when managing personal finances, the ability to calculate expenses, savings, and investments is crucial for making sound financial decisions.Furthermore, mathematics is the language of science and technology. It is the foundation of various scientific and technological advancements, from engineering and architecture to computer science and data analysis. Without a solid understanding of mathematics, it would be nearly impossible to comprehend and contribute to the advancements in these fields. For instance, in the field of computer programming, mathematical concepts such as algorithms and logic are essential for writing efficient and error-free code.In addition, mathematics is closely linked to other disciplines, such as physics, chemistry, and economics. Many principles and theories in these fields rely heavily on mathematical concepts and formulas. For instance, in physics, mathematical equations are used to describe the behavior of particles and the laws of motion. In economics, mathematical models are employed to analyze market trends and predict future outcomes. Therefore, a strong foundation in mathematics is essential for gaining a deeper understanding of these subjects.Moreover, mathematics fosters critical thinking and creativity. It encourages us to explore different approaches to problem-solving and to think outside the box. This notonly enhances our analytical skills, but also stimulates our creativity and innovation. For example, in the field of art and design, mathematical principles such as symmetry, proportion, and geometry are utilized to create aesthetically pleasing and structurally sound works.In conclusion, mathematics is undeniably important in our lives. It shapes our logical thinking, problem-solving abilities, and cognitive development. It serves as the backbone of scientific and technological advancements, and it is closely intertwined with other disciplines. Furthermore, it fosters critical thinking and creativity, which are essential skills for success in the modern world. Therefore, it is crucial for individuals to recognize the significance of mathematics and to strive for a strong foundation in this subject. By doing so, we can not only excel academically and professionally, but also enrich our overall quality of life.。

symmetry词根

symmetry词根

symmetry词根单词:symmetry1.1词性:名词1.2中文释义:对称;匀称;整齐1.3英文释义:The quality of being made up of exactly similar parts facing each other or around an axis.1.4相关词汇:symmetrical(形容词,对称的)、asymmetry(名词,不对称)、symmetrically(副词,对称地)2. 起源与背景2.1词源:它源自于希腊语“symmetria”,由“s yn -”(一起、共同)和“metron”(测量)组成,最初的意义是关于比例和和谐的测量关系。

2.2趣闻:在古希腊建筑中,symmetry有着极高的地位。

像帕特农神庙,其建筑结构处处体现着对称美。

从正面看,柱子的排列、三角楣的设计等都是左右对称的,这种对称不仅体现了当时的审美观念,也被认为是一种体现宇宙秩序的方式。

3. 常用搭配与短语3.1短语:(1)axis of symmetry:对称轴例句:The line in the middle of the figure is the axis of symmetry.翻译:图形中间的这条线是对称轴。

(2)symmetry breaking:对称破缺例句:Symmetry breaking is an important concept in physics.翻译:对称破缺是物理学中的一个重要概念。

(3)bilateral symmetry:两侧对称例句:Most animals have bilateral symmetry.翻译:大多数动物都有两侧对称的特征。

4. 实用片段(1). "Look at this butterfly, its wings have such perfect symmetry." Tom said to his little sister. "Yeah, it's really beautiful." His sister replied.翻译:“看这只蝴蝶,它的翅膀有着如此完美的对称。

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An approach to Symmetry Breaking in DistributedConstraint Satisfaction ProblemsRoland Martin1and David A.Burke21SAF AG,Simulation,Analysis and Forecastingand Darmstadt University of Technology Algorithmics Group,Germany2Centre for Telecommunications Value-chain Researchand Cork Constraint Computation Centre,Dept.of Computer Science,University College Cork,Ireland martin@rmatik.tu-darmstadt.de, d.burke@4c.ucc.ieAbstract.Symmetry breaking in Distributed Constraint Satisfaction Problems(DisCSPs)has,to the best of our knowledge,not been investigated.In this paper,we show that most symmetries in DisCSPs are actually weak symmetries,and wedemonstrate how weak symmetry breaking techniques can be applied to DisCSPs.1IntroductionIn Multi-agent Systems,many applications involve solving problems that are naturally distributed over a set of agents,e.g,in a disaster rescue scenario,multiple agents with interdependent plans need to have their task schedules coordinated[1].Further exam-ples include coordinating vehicle schedules in a transport logistics problem[2],or staff timetabling in large organisations with multiple departments[3].One technique for modelling and solving these problems is the Distributed Constraint Satisfaction Prob-lem(DisCSP)[4]formulism,which is an extension of the Constraint Satisfaction Prob-lem(CSP).DisCSP algorithms solve the problem in its natural distributed state search-ing for globally acceptable solutions while minimising communcation between agents.Symmetry breaking[5]has been shown to provide great benefits when solving cen-tralised CSPs.By identifying assignments to a problem that are symmetrically equiv-alent,large areas of the search space can be eliminated by considering only one as-signment taken from each equivalence set.Weak symmetries are a special case of sym-metries that act only on a subset of the variables and the weakly symmetric solutions satisfy only a subset of the constraints of the problem.Weak symmetries occur in many real-world problems such as planning,scheduling and model checking[6,7].If a CSP is distributed among several agents then each agent only has access to a subset of the variables and the constraints.If the subproblem of an agent contains a symmetry,two solutions that are symmetric for the agent may not be symmetric in the context of the larger global problem,i.e.the solutions may not be equivalent for other agents in the problem,thus the symmetry is weak.That means the symmetries of the agent cannot be broken since the agent does not know whether these solutions are symmetric for other agents.A modelling approach introduced in[8]allows weak symmetries to be broken without losing solutions.In this paper we will show how this approach can be applied to DisCSPs which represents thefirst method of symmetry breaking in DisCSPs.2Distributed Constraint Satisfaction ProblemA Distributed Constraint Satisfaction Problem consists of a set A ={a 1,a 2,...,a n }of agents ,and for each agent a i ,a set X i ={x i 1,x i 2,...,x im i }of variables it con-trols,such that ∀i =j X i ∩X j =∅.Each variable x ij has a corresponding domain D ij .X = X i is the set of all variables in the problem.C ={c 1,c 2,...,c t }is a set of con-straints .Each c k has a scope s (c k )⊆X .The agent scope ,a (c k ),of c k is the set of agents that c k acts upon:a (c k )={a i :X i ∩s (c k )=∅}.An agent a i is a neighbour of an agent a j if ∃c k :a i ,a j ∈a (c k ).For each agent a i ,p i ={x ij :∀c x ij ∈s (c )→s (c )⊆X i }is its private variables –variables which are not constrained by other agents’variables –and e i =X i \p i is its public variables –variables that have constraints with other agents.A global assignment ,is the selection of one value for each variable in X .A local assignment ,to an agent a i ,is an assignment to X i .A solution to a DisCSP is a global assignment such that no constraints are violated.The solution process,however,is restricted:each agent is responsible for the assignment of its own variables,and thus agents must communicate with each other in order to find a global solution.Asynchronous Backtracking (ABT)[4]is an asynchronous and distributed back-tracking algorithm for solving DisCSPs.Agents act concurrently without any global control.A priority order is first created over the agents.Then,higher priority agents send ok?messages,containing a proposed assignment of their public variables,to lower priority agents.When an agent receives an ok?message it adds this assignment to its current agent view ,which is its belief of what values are assigned to the other agents’variables.It then searches for a solution to its subproblem that is consistent with this agent view .If it finds a consistent solution,it sends its new assignment of its public vari-ables in an ok?message to lower priority agents.If it can find no consistent assignment,it sends a nogood message specifying the assignment(s)that are causing the conflict to the lowest priority agent involved in the conflict (other than itself).The search pro-gresses until a consistent global solution is found or the problem is proved infeasible.To search for a consistent local assignment to an agent’s subproblem,a centralised CSP solver can be used.To use symmetry breaking as part of this local solving process is difficult because:(i)solutions that are symmetric for one agent’s subproblem but that contain different assignments to the agent’s public variables may not be equivalent with regards to the global problem;and (ii)no single agent has a complete view of all variables and all constraints in the global problem.Since only an agent’s public variables affect the other agents in the problem,symmetry breaking can be used only if all solutions in an equivalence set have identical assignments to the agent’s public variables.However,if this is not the case it is not possible to break the symmetry without risking losing solutions.In Section 4,we propose the first steps in tackling this problem.3Weak SymmetryIf a CSP P has a subproblem P where P has a symmetry πthat P does not then πis called a weak symmetry on P (see [8]for a more formal definition).The challenge in weak symmetry breaking is to not lose solutions when breaking the symmetries that exist in a subproblem.P may contain several solutions to it that are symmetrical,how-ever,although a solution s to the subproblem P may be symmetrical to another solutions of the subproblem P ,the solutions may not be equivalent with respect to the entire problem P.Therefore we cannot discard solutions as readily as in regular symmetry breaking.We need a way to represent all these solutions in the search process if we want to break the symmetry.To do this,we use a modelling approach proposed in[8]that works by introducing additional variables called SymVars into a problem that can represent all solutions of an equivalence class.On these variables we state constraints that model the weak symme-try.The weak symmetry on P can then be broken by any desired symmetry breaking method.When solving the problem,wefirst search for a solution for the subproblem P .When a solution s to P is found we instantiate the SymVars and then attempt to extend this solution to P.If a conflict is detected,we backtrack on the SymVars tofind an equivalent solution to s(as opposed to searching for a new solution to P ).We then attempt to extend this new solution to P.Only if no permutation of s produces a feasible solution do we backtrack and search for a new solution that satisfies P .4Breaking Weak Symmetries in DisCSPsTo demonstrate how we can break weak symmetries in DisCSP,we artificially con-struct a distributed magic square problem.In the magic square problem,the numbers 1,...,n2have to be assigned to a n×n square such that the sum of the numbers in each row,in each column and in both main diagonals are equal.The value m for thissum necessarily satisfies m=n3+n2.In our distributed scenario(Figure1)3,agent Aowns all variables that make up a magic square but for its particular local subproblem it is only interested in enforcing row and column constraints.Agent B,holds variables that are constrained to be equal to the diagonal and anti-diagonal variables of agent A. Furthermore agent B will enforce the diagonal and anti-diagonal constraints on its vari-ables.This can be seen as an instance of a multi-agent agreement problem where agents need to agree on the values of public variables that are bound by equality constraints, considering their own private internal variables and constraints4.We can apply weak symmetry breaking techniques on the resulting problem.Con-sider the column symmetries of agent A’s subproblem.Any solution found that satisfies the row and column constraints can be permuted by changing the order of the columns to produce n!symmetrical solutions.This symmetry can be broken by adding a con-straint that orders the columns such that thefirst element in a column is less than the first element of the following column-thus,only one solution of each equivalence set will be found.However,in the DisCSP case,we can not afford to lose these equivalent 3We use afictional distributed scenario of this well known problem in order to easily and clearly describe our approach.The techniques we describe are equally applicable to real world plan-ning and scheduling scenarios with multiple agents,each with large subproblems.4In a DisCSP each agent owns and chooses assignments for its own independent set of vari-ables.In this example the equality constraints ensure that it is beneficial for the agents to set their public variables identically,but there are still two sets of independent variables,i.e.the variables are not shared.In the general case,public variables may be bound by any type of constraint,not just equality constraints.Fig.1.DisCSP formulation of Magic Square problem.Agent A contains all the variables of the square and will enforce row and column constraints on these.Agent B contains variables that are constrained to be equal to the diagonal variables of Agent A(dashed lines indicate equality constraints)and will enforce the diagonal and anti-diagonal constraints on its variables.(a)(b)Fig.2.Magic square:n=4,m=34.(a)-by introducing SymVars agent A can break the column symmetry of its original subproblem.(b)-equivalent solutions can then be generated using the SymVars tofind a permutation that is also valid for agent B’s constraints.solutions.It is possible that one valid solution found for agent A can not be extended to a valid solution in agent B,while an equivalent solution can be.The challenge we face is how to enforce symmetry without losing solutions that may be required by other agents in the problem.To do this,we introduce a SymVar for each column to agent A to represent the permutations of a solution to its subproblem (Figure2).In our example,an assignment to the SymVars will represent one particular permutation of the columns of a solution,and the SymVars will be constrained to be alldifferent.We also introduce variables to represent the permuted solution projected on the agent’s public variables.We consider an example execution of ABT and assume that agent A is assigned a higher priority than agent B.Agent A will search for a solu-tion to the variables of its magic square(using column symmetry breaking)observing the row and column constraints(Figure2(a)).Next the SymVars are assigned,which in turn leads to an assignment of the new projected public variables.Agent A will send the assignment of its public variables to agent B.Agent B’s public constraints require that its assignments to its variables must be equal to the corresponding public vari-ables of agent A.However,by enforcing this it will not have a solution consistent with its internal constraints,i.e.the diagonal and anti-diagonal constraints are not satisfied. Therefore,it sends a nogood to agent A and agent A will add a constraint to its sub-problem that rules out this assignment.Agent A will then select a new solution using its SymVars,i.e.instead of searching for a new solution to its magic square,it justfinds a new assignment to its SymVars,which leads to a new assignment to the projected public variables(Figure2(b)).A new non-symmetric solution for the agent’s internal problem will only be searched for once all symmetrical solutions have been exhausted.In our example,the new permutation of the original solution produces an assignment to the public variables that allow agent B’s constraints to also be satisfied,and so a global solution has been found.The benefit of this approach is thatfinding a new assignment to the SymVars is much less expensive than searching for a new solution to the magic square.We can break symmetries in a standard way,while the SymVars will ensure that equivalent solutions can be generated if required.5Conclusions and OutlookWe have showed that most symmetries in DisCSPs are actually weak symmetries and have applied fruitfully a weak symmetry breaking approach to DisCSPs.This is the first symmetry breaking approach to DisCSPs as far as we know.We demonstrated the approach using the magic square problem modelled as a DisCSP.This paper represents our initial investigations into this issue and future work will focus on implementing and evaluating the approach using state-to-the-art DisCSP algorithms.6AcknowledgementsD.Burke is supported by Science Foundation Ireland under Grant No.03/CE3/I405as part of the Centre for Telecommunications Value-Chain Research(CTVR).The authors would like to thank the reviewers for useful comments.References1.Sultanik,E.A.,Modi,P.J.,Regli,W.C.:Constraint propagation for domain bounding in c-taems task scheduling.In:Proc.CP.(2006)756–7602.Calisti,M.,Neagu,N.:Constraint satisfaction techniques and software agents.In:Proc.Agents and Constraints Workshop,AIIA.(2004)3.Meisels,A.,Kaplansky,E.:Scheduling agents-distributed timetabling problems(disttp).In:Proc.PATAT.(2002)166–1774.Yokoo,M.,Hirayama,K.:Algorithms for distributed constraint satisfaction:A review.Au-tonomous Agents and Multi-Agent Systems3(2)(2000)185–2075.Gent,I.P.,Petrie,K.E.,Puget,J.F.:Symmetry in constraint programming.In:Handbook ofConstraint Programming.F.Rossi and P.van Beek and T.Walsh(2006)6.Gregory,P.:Almost–symmetry in planning.In:Proc.SymNet Workshop on Almost-Symmetry in Search.(2005)14–167.Donaldson,A.:Partial symmetry in model checking.In:Proc.SymNet Workshop on Almost-Symmetry in Search.(2005)17–218.Martin,R.:The challenge of exploiting weak symmetries.In:Proc.CSCLP.(2005)149–163。

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