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PREFACE
a modified TDGL scheme which is unequivocally valid for the much more general
case of finite-gap materials! This derivation combines the very general equations
applicable to equilibrium (Chapter 1) and nonequilibrium (Chapter 3) supercon-
ductivity. Both the Keldysh and Eliashberg-Gor’kov analytical continuations tech-
nique are exploited to prove the same results are achieved.
It is really amazing how nicely these two mathematically very different tools
yield precisely the same results! Given this equivalence of the results, the reader
might wonder which is preferable from a practical point of view. We conclude that
for the phenomena which have already been treated in equilibrium in the Matsubara
technique it is faster to apply the analytical continuation method. In general,
Keldysh’s method is more straightforward.
Since nonequilibrium superconductivity exploits some concepts which do not
occur in equilibrium case, such as the longitudinal electric field penetration depth
and branch imbalance potential, we devoted a special discussion (Chapter 8) to
collective oscillations. These are formally out of the range of applicability of TDGL.
The kinetic equations, which follow from the general nonequilibrium equations
(Chapter 4), provided the mathematical basis to discuss various nonequilibrium
effects in superconductors. We tried everywhere to treat nonequilibrium electrons
and phonons on an equal footing. Thus in parallel to enhancement of the order
parameter (Chapter 5), we considered the accompanying phonon deficit effect
(Chapter 6). In this two chapters the collision integrals, which traditionally serve
to describe the relaxation processes, were used also to describe the sources of
nonequilibrium deviation of both electrons and phonons.
The behavior of nonequilibrium Josephson junctions and the more novel but
closely related phase-slip centers are treated in detail in Chapters 10 and 9
respectively. Attention is paid to both the phonon and electron components.
Irradiation by lasers is a traditional method for creating a nonequilibrium
superconducting state (see Chapter 11). In Chapter 12 we considered the inverse
problem: the ability of a superconductor in a nonequilibrium state to act as a
coherent phonon or photon generator. This laser-like source behaviors have not yet
been experimentally confirmed. However, we hoped our discussion will encourage
their demonstration.
The final chapters of the book, 13 and 14, discuss thermoelectricity. This topic
is one of the most complex, subtle featured and thus intellectually captivating in
solid state physics. The addition of superconductivity to the discussion creates even
more opportunity to be excited by thermoelectricity.
The book's initial chapter includes an introduction to the theory of supercon-
ductivity for those readers not already acquainted with it. The treatment is very
concise but covers the most important physical concepts which will later be
assumed to be familiar to the reader. The mathematical constructs of quantum field
theory are assumed to need no explanation.