Abstract:
We consider phase transitions in crystals with a strong interband
electron–phonon interaction. We investigate the thermodynamic potential of
the system using the method of temperature Green's functions, which takes
quantum and thermal fluctuations into account. We show that in the absence of
striction, these phase transitions are realized as a sequence of second-order
phase transitions in each of which the thermodynamic potential has
a logarithmic singularity, as in the Onsager model. This suggests that this
singularity is characteristic of all second-order phase transitions. We show
that the energy preference of the transition to the ordered phase is ensured
by the electron coupling to coherent displacements of ions along normal
coordinates of the phonon modes. We calculate the limit value of the energy
decrease in the ordered phase compared with the symmetric phase as
$T\to0$ K.