162 research outputs found
A nonlinear model dynamics for closed-system, constrained, maximal-entropy-generation relaxation by energy redistribution
We discuss a nonlinear model for the relaxation by energy redistribution
within an isolated, closed system composed of non-interacting identical
particles with energy levels e_i with i=1,2,...,N. The time-dependent
occupation probabilities p_i(t) are assumed to obey the nonlinear rate
equations tau dp_i/dt=-p_i ln p_i+ alpha(t)p_i-beta(t)e_ip_i where alpha(t) and
beta(t) are functionals of the p_i(t)'s that maintain invariant the mean energy
E=sum_i e_ip_i(t) and the normalization condition 1=sum_i p_i(t). The entropy
S(t)=-k sum_i p_i(t) ln p_i(t) is a non-decreasing function of time until the
initially nonzero occupation probabilities reach a Boltzmann-like canonical
distribution over the occupied energy eigenstates. Initially zero occupation
probabilities, instead, remain zero at all times. The solutions p_i(t) of the
rate equations are unique and well-defined for arbitrary initial conditions
p_i(0) and for all times. Existence and uniqueness both forward and backward in
time allows the reconstruction of the primordial lowest entropy state. The time
evolution is at all times along the local direction of steepest entropy ascent
or, equivalently, of maximal entropy generation. These rate equations have the
same mathematical structure and basic features of the nonlinear dynamical
equation proposed in a series of papers ended with G.P.Beretta, Found.Phys.,
17, 365 (1987) and recently rediscovered in S. Gheorghiu-Svirschevski,
Phys.Rev.A, 63, 022105 and 054102 (2001). Numerical results illustrate the
features of the dynamics and the differences with the rate equations recently
considered for the same problem in M.Lemanska and Z.Jaeger, Physica D, 170, 72
(2002).Comment: 11 pages, 7 eps figures (psfrag use removed), uses subeqn, minor
revisions, accepted for Physical Review
Asymptotics of Quantum Relative Entropy From Representation Theoretical Viewpoint
In this paper it was proved that the quantum relative entropy can be asymptotically attained by Kullback Leibler divergences of
probabilities given by a certain sequence of POVMs. The sequence of POVMs
depends on , but is independent of the choice of .Comment: LaTeX2e. 8 pages. The title was changed from "Asymptotic Attainment
for Quantum Relative Entropy
Equilibrium states and their entropy densities in gauge-invariant C*-systems
A gauge-invariant C*-system is obtained as the fixed point subalgebra of the
infinite tensor product of full matrix algebras under the tensor product
unitary action of a compact group. In the paper, thermodynamics is studied on
such systems and the chemical potential theory developed by Araki, Haag,
Kastler and Takesaki is used. As a generalization of quantum spin system, the
equivalence of the KMS condition, the Gibbs condition and the variational
principle is shown for translation-invariant states. The entropy density of
extremal equilibrium states is also investigated in relation to macroscopic
uniformity.Comment: 20 pages, revised in March 200
On the comparison of volumes of quantum states
This paper aims to study the \a-volume of \cK, an arbitrary subset of the
set of density matrices. The \a-volume is a generalization of the
Hilbert-Schmidt volume and the volume induced by partial trace. We obtain
two-side estimates for the \a-volume of \cK in terms of its Hilbert-Schmidt
volume. The analogous estimates between the Bures volume and the \a-volume
are also established. We employ our results to obtain bounds for the
\a-volume of the sets of separable quantum states and of states with positive
partial transpose (PPT). Hence, our asymptotic results provide answers for
questions listed on page 9 in \cite{K. Zyczkowski1998} for large in the
sense of \a-volume.
\vskip 3mm PACS numbers: 02.40.Ft, 03.65.Db, 03.65.Ud, 03.67.M
A set-valued framework for birth-and-growth process
We propose a set-valued framework for the well-posedness of birth-and-growth
process. Our birth-and-growth model is rigorously defined as a suitable
combination, involving Minkowski sum and Aumann integral, of two very general
set-valued processes representing nucleation and growth respectively. The
simplicity of the used geometrical approach leads us to avoid problems arising
by an analytical definition of the front growth such as boundary regularities.
In this framework, growth is generally anisotropic and, according to a
mesoscale point of view, it is not local, i.e. for a fixed time instant, growth
is the same at each space point
Free energy density for mean field perturbation of states of a one-dimensional spin chain
Motivated by recent developments on large deviations in states of the spin
chain, we reconsider the work of Petz, Raggio and Verbeure in 1989 on the
variational expression of free energy density in the presence of a mean field
type perturbation. We extend their results from the product state case to the
Gibbs state case in the setting of translation-invariant interactions of finite
range. In the special case of a locally faithful quantum Markov state, we
clarify the relation between two different kinds of free energy densities (or
pressure functions).Comment: 29 pages, Section 5 added, to appear in Rev. Math. Phy
A matrix interpolation between classical and free max operations: I. The univariate case
Recently, Ben Arous and Voiculescu considered taking the maximum of two free
random variables and brought to light a deep analogy with the operation of
taking the maximum of two independent random variables. We present here a new
insight on this analogy: its concrete realization based on random matrices
giving an interpolation between classical and free settings.Comment: 14 page
Large Deviations for a Non-Centered Wishart Matrix
We investigate an additive perturbation of a complex Wishart random matrix
and prove that a large deviation principle holds for the spectral measures. The
rate function is associated to a vector equilibrium problem coming from
logarithmic potential theory, which in our case is a quadratic map involving
the logarithmic energies, or Voiculescu's entropies, of two measures in the
presence of an external field and an upper constraint. The proof is based on a
two type particles Coulomb gas representation for the eigenvalue distribution,
which gives a new insight on why such variational problems should describe the
limiting spectral distribution. This representation is available because of a
Nikishin structure satisfied by the weights of the multiple orthogonal
polynomials hidden in the background.Comment: 40 page
Statistical Inference, Distinguishability of Quantum States, And Quantum Entanglement
We argue from the point of view of statistical inference that the quantum
relative entropy is a good measure for distinguishing between two quantum
states (or two classes of quantum states) described by density matrices. We
extend this notion to describe the amount of entanglement between two quantum
systems from a statistical point of view. Our measure is independent of the
number of entangled systems and their dimensionality.Comment: 11 pages no figures, to appear in Phys. Rev.
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