Statistical Physics, Part 1A lucid presentation of statistical physics and thermodynamics which develops from the general principles to give a large number of applications of the theory. |
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Page 450
... transition point of the second kind has a continuous change of ʼn to zero . The absence of any discontinuous change of state at a phase transition point of the second kind has the result that the thermodynamic functions of the state of ...
... transition point of the second kind has a continuous change of ʼn to zero . The absence of any discontinuous change of state at a phase transition point of the second kind has the result that the thermodynamic functions of the state of ...
Page 462
... transition point itself , the crystal must have the symmetry Go , i.e. the equilibrium values of the n " ) must be zero . It is evident that Ø can ... transition point , and 462 Phase Transitions of the Second Kind and Critical Phenomena.
... transition point itself , the crystal must have the symmetry Go , i.e. the equilibrium values of the n " ) must be zero . It is evident that Ø can ... transition point , and 462 Phase Transitions of the Second Kind and Critical Phenomena.
Page 505
... transition point . The expansion of ( t ) in powers of t = T - T , near the transition point includes a singular term as well as the regular part . Here we are interested only in the singular term , the regular part being simply ...
... transition point . The expansion of ( t ) in powers of t = T - T , near the transition point includes a singular term as well as the regular part . Here we are interested only in the singular term , the regular part being simply ...
Contents
Elementary excitations in a quantum Fermi liquid | 1 |
Interaction of quasiparticles | 2 |
Magnetic susceptibility of a Fermi liquid | 3 |
Copyright | |
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atoms axis body Bravais lattice calculate cell chemical potential classical coefficients components concentration condition constant coordinates correlation function corresponding critical point crystal denote density depends derivative determined electron elements entropy equal equation expansion expression Fermi field fluctuations formula free energy frequency gases Gibbs distribution given gives Hamiltonian Hence ideal gas integral interaction irreducible representations liquid macroscopic magnetic matrix mean square mean value molecule momenta momentum motion N₁ number of particles obtain order parameter P₁ partition function phase transition phonon plane pressure PROBLEM properties Quantum Mechanics reciprocal lattice regarded relation result rotational second kind solid solution solvent space group specific heat statistical substance Substituting subsystem suffix surface symmetry temperature theory thermal thermodynamic potential thermodynamic quantities tion total number transformation transition point vapour variables velocity vibrations volume zero ӘР