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Preface | ||
Acknowledgements | ||
1 | The laws of thermodynamics | 1 |
1.1 | The thermodynamic system and processes | 1 |
1.2 | The zeroth law of thermodynamics | 1 |
1.3 | The thermal equation of state | 2 |
1.4 | The classical ideal gas | 4 |
1.5 | The quasistatic and reversible processes | 7 |
1.6 | The first law of thermodynamics | 7 |
1.7 | The heat capacity | 8 |
1.8 | The isothermal and adiabatic processes | 10 |
1.9 | The enthalpy | 12 |
1.10 | The second law of thermodynamics | 12 |
1.11 | The Carnot cycle | 14 |
1.12 | The thermodynamic temperature | 15 |
1.13 | The Carnot cycle of an ideal gas | 19 |
1.14 | The Clausius inequality | 22 |
1.15 | The entropy | 24 |
1.16 | General integrating factors | 26 |
1.17 | The integrating factor and cyclic processes | 28 |
1.18 | Hausen's cycle | 30 |
1.19 | Employment of the second law of thermodynamics | 31 |
1.20 | The universal integrating factor | 32 |
2 | Thermodynamics relations | 38 |
2.1 | Thermodynamic potentials | 38 |
2.2 | Maxwell relations | 41 |
2.3 | The open system | 42 |
2.4 | The Clausius-Clapeyron equation | 44 |
2.5 | The van der Waals equation | 46 |
2.6 | The grand potential | 48 |
3 | The ensemble theory | 50 |
3.1 | Microstate and macrostate | 50 |
3.2 | Assumption of equal a priori probabilities | 52 |
3.3 | The number of microstates | 52 |
3.4 | The most probable distribution | 53 |
3.5 | The Gibbs paradox | 55 |
3.6 | Resolution of the Gibbs paradox: quantum ideal gases | 56 |
3.7 | Canonical ensemble | 58 |
3.8 | Thermodynamic relations | 61 |
3.9 | Open systems | 63 |
3.10 | The grand canonical distribution | 63 |
3.11 | The grand partition function | 64 |
3.12 | The ideal quantum gases | 66 |
4 | System Hamiltonians | 69 |
4.1 | Representations of the state vectors | 69 |
4.2 | The unitary transformation | 76 |
4.3 | Representations of operators | 77 |
4.4 | Number representation for the harmonic oscillator | 78 |
4.5 | Coupled oscillators: the linear chain | 82 |
4.6 | The second quantization for bosons | 84 |
4.7 | The system of interacting fermions | 88 |
4.8 | Some examples exhibiting the effect of Fermi-Dirac statistics | 91 |
4.9 | The Heisenberg exchange Hamiltonian | 94 |
4.10 | The electron-phonon interaction in a metal | 95 |
4.11 | The dilute Bose gas | 99 |
4.12 | The spin-wave Hamiltonian | 101 |
5 | The density matrix | 106 |
5.1 | The canonical partition function | 106 |
5.2 | The trace invariance | 107 |
5.3 | The perturbation expansion | 108 |
5.4 | Reduced density matrices | 110 |
5.5 | One-site and two-site density matrices | 111 |
5.6 | The four-site reduced density matrix | 114 |
5.7 | The probability distribution functions for the Ising model | 121 |
6 | The cluster variation method | 127 |
6.1 | The variational principle | 127 |
6.2 | The cumulant expansion | 128 |
6.3 | The cluster variation method | 130 |
6.4 | The mean-field approximation | 131 |
6.5 | The Bethe approximation | 134 |
6.6 | Four-site approximation | 137 |
6.7 | Simplified cluster variation methods | 141 |
6.8 | Correlation function formulation | 144 |
6.9 | The point and pair approximations in the CFF | 145 |
6.10 | The tetrahedron approximation in the CFF | 147 |
7 | Infinite-series representations of correlation functions | 153 |
7.1 | Singularity of the correlation functions | 153 |
7.2 | The classical values of the critical exponent | 154 |
7.3 | An infinite-series representation of the partition function | 156 |
7.4 | The method of Pade approximants | 158 |
7.5 | Infinite-series solutions of the cluster variation method | 161 |
7.6 | High temperature specific heat | 165 |
7.7 | High temperature susceptibility | 167 |
7.8 | Low temperature specific heat | 169 |
7.9 | Infinite series for other correlation functions | 172 |
8 | The extended mean-field approximation | 175 |
8.1 | The Wentzel criterion | 175 |
8.2 | The BCS Hamiltonian | 178 |
8.3 | The s-d interaction | 184 |
8.4 | The ground state of the Anderson model | 190 |
8.5 | The Hubbard model | 197 |
8.6 | The first-order transition in cubic ice | 203 |
9 | The exact Ising lattice identities | 212 |
9.1 | The basic generating equations | 212 |
9.2 | Linear identities for odd-number correlations | 213 |
9.3 | Star-triangle-type relationships | 216 |
9.4 | Exact solution on the triangular lattice | 218 |
9.5 | Identities for diamond and simple cubic lattices | 221 |
9.6 | Systematic naming of correlation functions on the lattice | 221 |
10 | Propagation of short range order | 230 |
10.1 | The radial distribution function | 230 |
10.2 | Lattice structure of the superionic conductor [alpha]Agl | 232 |
10.3 | The mean-field approximation | 234 |
10.4 | The pair approximation | 235 |
10.5 | Higher order correlation functions | 237 |
10.6 | Oscillatory behavior of the radial distribution function | 240 |
10.7 | Summary | 244 |
11 | Phase transition of the two-dimensional Ising model | 246 |
11.1 | The high temperature series expansion of the partition function | 246 |
11.2 | The Pfaffian for the Ising partition function | 248 |
11.3 | Exact partition function | 253 |
11.4 | Critical exponents | 259 |
App. 1 | The gamma function | 261 |
App. 2 | The critical exponent in the tetrahedron approximation | 265 |
App. 3 | Programming organization of the cluster variation method | 269 |
App. 4 | A unitary transformation applied to the Hubbard Hamiltonian | 278 |
App. 5 | Exact Ising identities on the diamond lattice | 281 |
References | 285 | |
Bibliography | 289 | |
Index | 291 |
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