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As our title suggests, there are two aspects in the subject of this
book. The first is the mathematical investigation of the dynamics
of infinite systems of in teracting particles and the description
of the time evolution of their states. The second is the rigorous
derivation of kinetic equations starting from the results of the
aforementioned investigation. As is well known, statistical
mechanics started in the last century with some papers written by
Maxwell and Boltzmann. Although some of their statements seemed
statistically obvious, we must prove that they do not contradict
what me chanics predicts. In some cases, in particular for
equilibrium states, it turns out that mechanics easily provides the
required justification. However things are not so easy, if we take
a step forward and consider a gas is not in equilibrium, as is,
e.g., the case for air around a flying vehicle. Questions of this
kind have been asked since the dawn of the kinetic theory of gases,
especially when certain results appeared to lead to paradoxical
conclu sions. Today this matter is rather well understood and a
rigorous kinetic theory is emerging. The importance of these
developments stems not only from the need of providing a careful
foundation of such a basic physical theory, but also to exhibit a
prototype of a mathematical construct central to the theory of
non-equilibrium phenomena of macroscopic size."
This monograph is devoted to quantum statistical mechanics. It can
be regarded as a continuation of the book "Mathematical Foundations
of Classical Statistical Mechanics. Continuous Systems" (Gordon
& Breach SP, 1989) written together with my colleagues V. I.
Gerasimenko and P. V. Malyshev. Taken together, these books give a
complete pre sentation of the statistical mechanics of continuous
systems, both quantum and classical, from the common point of view.
Both books have similar contents. They deal with the investigation
of states of in finite systems, which are described by infinite
sequences of statistical operators (reduced density matrices) or
Green's functions in the quantum case and by infinite sequences of
distribution functions in the classical case. The equations of
state and their solutions are the main object of investigation in
these books. For infinite systems, the solutions of the equations
of state are constructed by using the thermodynamic limit
procedure, accord ing to which we first find a solution for a
system of finitely many particles and then let the number of
particles and the volume of a region tend to infinity keeping the
density of particles constant. However, the style of presentation
in these books is quite different."
As our title suggests, there are two aspects in the subject of this
book. The first is the mathematical investigation of the dynamics
of infinite systems of in teracting particles and the description
of the time evolution of their states. The second is the rigorous
derivation of kinetic equations starting from the results of the
aforementioned investigation. As is well known, statistical
mechanics started in the last century with some papers written by
Maxwell and Boltzmann. Although some of their statements seemed
statistically obvious, we must prove that they do not contradict
what me chanics predicts. In some cases, in particular for
equilibrium states, it turns out that mechanics easily provides the
required justification. However things are not so easy, if we take
a step forward and consider a gas is not in equilibrium, as is,
e.g., the case for air around a flying vehicle. Questions of this
kind have been asked since the dawn of the kinetic theory of gases,
especially when certain results appeared to lead to paradoxical
conclu sions. Today this matter is rather well understood and a
rigorous kinetic theory is emerging. The importance of these
developments stems not only from the need of providing a careful
foundation of such a basic physical theory, but also to exhibit a
prototype of a mathematical construct central to the theory of
non-equilibrium phenomena of macroscopic size."
This monograph is devoted to quantum statistical mechanics. It can
be regarded as a continuation of the book "Mathematical Foundations
of Classical Statistical Mechanics. Continuous Systems" (Gordon
& Breach SP, 1989) written together with my colleagues V. I.
Gerasimenko and P. V. Malyshev. Taken together, these books give a
complete pre sentation of the statistical mechanics of continuous
systems, both quantum and classical, from the common point of view.
Both books have similar contents. They deal with the investigation
of states of in finite systems, which are described by infinite
sequences of statistical operators (reduced density matrices) or
Green's functions in the quantum case and by infinite sequences of
distribution functions in the classical case. The equations of
state and their solutions are the main object of investigation in
these books. For infinite systems, the solutions of the equations
of state are constructed by using the thermodynamic limit
procedure, accord ing to which we first find a solution for a
system of finitely many particles and then let the number of
particles and the volume of a region tend to infinity keeping the
density of particles constant. However, the style of presentation
in these books is quite different.
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