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内容简介

For this new edition， each chapter was revised and improved， typos corrected and figures added， some in response to many helpful comments on the first edition. We especially thank Professor Milton W. Cole for his correction of a factor 2 in the specific heat of a 1D hard-core Bose gas. Additionally， solutions to some representative problems have been included in an Appendix.
But， more t.han mere revision and expansion of the material， it is the wit and knowledge of a new co-author that has greatly improved the present text. Thanks to this couaboration the topics of renormalization group and Monte-Carlo numerical techniques could be treated on a par with more conventional elements of statistical thermodynamics. The addition of these important subjects and the expansion of topics that previously had been just many-body theory and phase transitions. We present this new edition in the hope it will better serve the contemporary student while offering to the instructor a wider， more useful choice of lecture materials.

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目录

Preface to Second Edition
Preface to First Edition
Introduction: Theories of Thermodynamics, Kinetic Theory and
Statistical Mechanics
Chapter 1 Elementary Concepts in Statistics and Probability
1.0.Random Variables and Their Distributions
1.1.The Binomial Distribution
1.2.Length of a Winning Streak
1.3.Brownian Motion and the Random Walk
1.4.Poisson versus Normal （Gaussian） Distributions
1.5.Central Limit Theorem （CLT）
1.6.Multinomial Distributions, Statistical Thermodynamics
1.7.The Barometer Equation
1.8.Other Distributions

Chapter 2 The Ising Model and the Lattice Gas
2.0.Physical Applications of the Binary Model
2.1.Some Background and Motivation
2.2.First-Principles Statistical Theory of Paramagnetism
2.3.More on Entropy and Energy
2.4.Some Other Relevant Thermodynamic Functions
2.5.Mean-Field Theory, Stable and Metastable Solutions
2.6.The Lattice Gas
2.7.The Nearest-Neighbor Chain: Thermodynamics in 1D
2.8.The Disordered Ising Chain
2.9.Other Magnetic Systems in One Dimension

Chapter 3 Elements of Thermodynamics
3.1.The Scope of Thermodynamics
3.2.Equations of State and Some Definitions
3.3.Maxwell Relations
3.4.Three Important Laws of Thermodynamics
3.5.The Second Derivatives of the Free Energy
3.6.Phase Diagrams for the van der Waals Gas
3.7.Clausius-Clapeyron Equation
3.8.Phase Transitions
3.9.The Carnot Cycle
3.10. Superconductivity

Chapter 4 Statistical Mechanics
4.0.An Axiomatic Approach and the Ergodic Hypothesis
4.1.The Formalism - and a False Start
4.2.Gibbs' Paradox and Its Remedy
4.3.The Gibbs Factor
4.4.The Grand Ensemble
4.5.Non-Ideal Gas and the 2-Body Correlation Function
4.6.The Virial Equation of State
4.7.Weakly Non-Ideal Gas
4.8. .Two-body Correlations
4.9.Configurational Partition Function in 1D
4.10. One Dimension versus Two
4.11. Two Dimensions versus Three: The Debye-Waller Factors
4.12. Specific Heat of Quasi-Ideal Dilute Atomic and Diatomic Gases
4.13. Nanophysics and Inhomogeneity

Chapter 5 The World of Bosons
5.0. Quantum "Statistics"
5.1.Two Types of Bosons and Their Operators
5.2.Number Representation and the Many-Body Problem
5.3.The Adiabatic Process and Conservation of Entropy
5.4.Many-Body Perturbations
5.5. Photons
……
Chapter 6 All About Fermions: Theories of Metals,Superconductors, Semiconductors
Chapter 7 Kinetic Theory
Chapter 8 The Transfer Matrix
Chapter 9 Monte Carlo and Other Computer Simulation Methods
Chapter 10 Critical Phenomena and the Renormalization Group
Chapter 11 Some Uses of Quantum Field Theory in Statistical Physics

前言/序言

物理学经典教材：统计力学（第2版） [Statistical Mechanics Made Simple 2nd Edition] 电子书 下载 mobi epub pdf txt

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买的书印刷质量还不错，

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　　同时，人们能够很容易理解没有观测电子环绕原子核的轨道的方法。第二个步骤在于显示一个不绕原子核运动而是离开原子的波包，因为第一个光量子已将电子从原子中打出。如果γ射线的波长远小于原子的大小，γ射线的光量子的动量将远大于电子的原始动量。因此，第一个光量子足以从原子中打出电子，并且人们决不能观测到电子轨道中另外的点；因此，也就没有通常意义的轨道了。下一次观测——第三个步骤——将显示电子离开原子的路线。两次相继观测之间所发生的事情，一般是完全无法描述的。当然，人们总想这样说：在两次观测之间，电子必定要处在某些地方，因而必定也描绘出某种路线或轨道，即使不可能知道是怎样一条路线。这在经典物理学中是一个合理的推论。但是，在量子论中，我们将在后面看出，这是语言的不合理的误用。我们可以暂时不去管这个警告究竟是指我们谈论原子事件的方法还是指原子事件本身，究竟它所涉及的是认识论还是本体论。但在任何情况下，我们对原子粒子的行为作任何陈述时，措辞都必须非常小心。

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这是一本入门级的统计力学书籍。

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内容丰富，可根据需要阅读。

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　　当量子论中的几率函数已在初始时间通过观测决定了以后，人们就能够从量子论定律计算出以后任何时间的几率函数，并能由此决定一次测量给出受测量的某一特殊值的几率。例如，我们能预测以后某一时间在云室中某一给定点发现电子的几率。应当强调指出，无论如何，几率函数本身并不代表事件在时间过程中的经过。它只代表一些事件的倾向和我们对这些事件的知识。只有当满足一个主要条件时：例如作了决定系统的某种性质的新测量时，几率函数才能和实在联系起来。只有那时，几率函数才容许我们计算新测量的可能结果。而测量结果还是用经典物理学的术语叙述的。　

评分☆☆☆☆☆

　　当量子论中的几率函数已在初始时间通过观测决定了以后，人们就能够从量子论定律计算出以后任何时间的几率函数，并能由此决定一次测量给出受测量的某一特殊值的几率。例如，我们能预测以后某一时间在云室中某一给定点发现电子的几率。应当强调指出，无论如何，几率函数本身并不代表事件在时间过程中的经过。它只代表一些事件的倾向和我们对这些事件的知识。只有当满足一个主要条件时：例如作了决定系统的某种性质的新测量时，几率函数才能和实在联系起来。只有那时，几率函数才容许我们计算新测量的可能结果。而测量结果还是用经典物理学的术语叙述的。　

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