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 159
... Bose distribution Let us now consider the statistics obeyed by an ideal gas consisting of particles described by symmetrical wave functions , namely Bose statistics or Bose - Einstein statistics . * The occupation numbers of the quantum ...
... Bose distribution Let us now consider the statistics obeyed by an ideal gas consisting of particles described by symmetrical wave functions , namely Bose statistics or Bose - Einstein statistics . * The occupation numbers of the quantum ...
Page 160
... Bose statistics ( or , as it is called for brevity , a Bose gas ) . It differs from the Fermi distri- bution function in the sign of unity in the denominator . Like that function , it tends of course to the Boltzmann distribution ...
... Bose statistics ( or , as it is called for brevity , a Bose gas ) . It differs from the Fermi distri- bution function in the sign of unity in the denominator . Like that function , it tends of course to the Boltzmann distribution ...
Page 162
... Bose gas in the impor- tant limiting case where the number of particles in each quantum state is large ( so that N , ≫ G1 , ñ ; ≫ 1 ) . We know from quantum mechanics ... Bose Distributions 56 Fermi and Bose gases of elementary particles.
... Bose gas in the impor- tant limiting case where the number of particles in each quantum state is large ( so that N , ≫ G1 , ñ ; ≫ 1 ) . We know from quantum mechanics ... Bose Distributions 56 Fermi and Bose gases of elementary particles.
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