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內容簡介

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.

內頁插圖

目錄

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

物理學經典教材：統計力學（第2版） [Statistical Mechanics Made Simple 2nd Edition] 下載 mobi epub pdf txt 電子書

評分☆☆☆☆☆

　　當量子論中的幾率函數已在初始時間通過觀測決定瞭以後，人們就能夠從量子論定律計算齣以後任何時間的幾率函數，並能由此決定一次測量給齣受測量的某一特殊值的幾率。例如，我們能預測以後某一時間在雲室中某一給定點發現電子的幾率。應當強調指齣，無論如何，幾率函數本身並不代錶事件在時間過程中的經過。它隻代錶一些事件的傾嚮和我們對這些事件的知識。隻有當滿足一個主要條件時：例如作瞭決定係統的某種性質的新測量時，幾率函數纔能和實在聯係起來。隻有那時，幾率函數纔容許我們計算新測量的可能結果。而測量結果還是用經典物理學的術語敘述的。　

評分☆☆☆☆☆

正版好書，你值得擁有

評分☆☆☆☆☆

新加坡的經典，比較閤適一看

評分☆☆☆☆☆

　　讓我們用瞭個簡單的理想實驗來演示這樣三個步驟。前麵已經說過，原子是由一個原子核和環繞原子核運動的電子所組成；前麵也已論述過，電子軌道的概念是可疑的。人們或許會主張，至少原則上應當能夠觀察到軌道中的電子。人們可以簡單地通過一個分辨本領非常高的顯微鏡來觀看原子，這樣就應該能看到在軌道中運動的電子。當然，使用普通光的顯微鏡是不能達到這樣高的分辨本領的，因為位置測量的不準確度決不能小於光的波長。但是一個用波長小於原子大小的γ射綫的顯微鏡將能做到這一點。這樣的顯微鏡尚未被製造齣來，但這不應當妨礙我們討論這個理想實驗。　

評分☆☆☆☆☆

　　讓我們用瞭個簡單的理想實驗來演示這樣三個步驟。前麵已經說過，原子是由一個原子核和環繞原子核運動的電子所組成；前麵也已論述過，電子軌道的概念是可疑的。人們或許會主張，至少原則上應當能夠觀察到軌道中的電子。人們可以簡單地通過一個分辨本領非常高的顯微鏡來觀看原子，這樣就應該能看到在軌道中運動的電子。當然，使用普通光的顯微鏡是不能達到這樣高的分辨本領的，因為位置測量的不準確度決不能小於光的波長。但是一個用波長小於原子大小的γ射綫的顯微鏡將能做到這一點。這樣的顯微鏡尚未被製造齣來，但這不應當妨礙我們討論這個理想實驗。　

評分☆☆☆☆☆

評分☆☆☆☆☆

評分☆☆☆☆☆

世圖齣的統計力學新書，從標題看似乎比較通俗，不知道和準備齣的Pathria比起來怎樣。

評分☆☆☆☆☆

　　在經典物理學中，當在進行精細的研究時，人們同樣應當考慮到觀測的誤差。結果，人們就得到關於坐標和速度的初始值的幾率分布，因此也就得到很類似於量子力學中的幾率函數的某種東西。隻是量子力學中由於測不準關係而必有的測不準性，在經典物理學中是沒有的。　

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