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<title>Физика низких температур, 2007, № 09</title>
<link href="http://dspace.nbuv.gov.ua:80/handle/123456789/118295" rel="alternate"/>
<subtitle/>
<id>http://dspace.nbuv.gov.ua:80/handle/123456789/118295</id>
<updated>2026-04-16T11:45:01Z</updated>
<dc:date>2026-04-16T11:45:01Z</dc:date>
<entry>
<title>Fine structure of critical opalescence spectra</title>
<link href="http://dspace.nbuv.gov.ua:80/handle/123456789/120940" rel="alternate"/>
<author>
<name>Sushko, M.Ya.</name>
</author>
<id>http://dspace.nbuv.gov.ua:80/handle/123456789/120940</id>
<updated>2017-06-14T00:07:15Z</updated>
<published>2007-01-01T00:00:00Z</published>
<summary type="text">Fine structure of critical opalescence spectra
Sushko, M.Ya.
The effect of the 1.5-scattering mechanism on the time and temperature behavior of the electric field&#13;
autocorrelation function for the light wave scattered from fluids has been studied for the case where the order-&#13;
parameter fluctuations obey the diffusion-like kinetics with spatially-dependent kinetic coefficient. The&#13;
leading contributions to the relevant static correlation functions of the order-parameter fluctuations were&#13;
obtained by using the Ginzburg–Landau model with a cubic term, and then evaluated with the use of the&#13;
Gaussian uncoupling for many-point correlation functions and the Ornstein–Zernicke form for the pair correlation&#13;
function. It is shown that the presence of the 1.5-scattering effects in the overall scattering pattern&#13;
may be detected in the form of a small but noticeable deviation from exponential decay of the total electric&#13;
field autocorrelation function registered experimentally near the critical point. Obtained with the standard&#13;
methods of analysis, the effective halfwidth of the corresponding spectrum can reveal a stronger temperature&#13;
dependence and a multiplicative renormalization as compared to the halfwidth of the spectrum of the&#13;
pair correlator.
</summary>
<dc:date>2007-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Nonequilibrium statistical operators for systems with finite lifetime</title>
<link href="http://dspace.nbuv.gov.ua:80/handle/123456789/120939" rel="alternate"/>
<author>
<name>Ryazanov, V.V.</name>
</author>
<id>http://dspace.nbuv.gov.ua:80/handle/123456789/120939</id>
<updated>2017-06-14T00:07:10Z</updated>
<published>2007-01-01T00:00:00Z</published>
<summary type="text">Nonequilibrium statistical operators for systems with finite lifetime
Ryazanov, V.V.
A family of nonequilibrium statistical operators (NSO) is introduced which differ by the system lifetime&#13;
distribution over which the quasiequilibrium (relevant) distribution is averaged. This changes the form of&#13;
the source in the Liouville equation, as well as the expressions for the kinetic coefficients, average fluxes,&#13;
and kinetic equations obtained with use of NSO. The difference from the Zubarev form of NSO is of the order&#13;
of the reciprocal lifetime of a system.
</summary>
<dc:date>2007-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>A Monte Carlo study of the Falicov–Kimball model in the perturbative regime</title>
<link href="http://dspace.nbuv.gov.ua:80/handle/123456789/120938" rel="alternate"/>
<author>
<name>Musiał, G.</name>
</author>
<author>
<name>Dębski, L.</name>
</author>
<author>
<name>Wojtkiewicz, J.</name>
</author>
<id>http://dspace.nbuv.gov.ua:80/handle/123456789/120938</id>
<updated>2017-06-14T00:07:15Z</updated>
<published>2007-01-01T00:00:00Z</published>
<summary type="text">A Monte Carlo study of the Falicov–Kimball model in the perturbative regime
Musiał, G.; Dębski, L.; Wojtkiewicz, J.
Finite-temperature properties of the Falicov–Kimball model on the square lattice have been studied in&#13;
the perturbative regime, i.e. for t/U &lt;&lt; 1, where t is the hopping constant and U denotes the Coulomb interaction&#13;
strength. In our study, we have determined the phase diagram of the model in the second-order of the&#13;
perturbation theory, where the antiferromagnetic Ising model in the magnetic field emerges. In the fourth-order,&#13;
where our model constitutes the Ising model with more complicated frustrated antiferromagnetic interactions,&#13;
the sketch of the phase diagram was established. The Monte Carlo method was employed and the behavior&#13;
of Binder cumulants based on the order parameters was analyzed to determine the type of ordering&#13;
and phase boundaries in the diagram.
</summary>
<dc:date>2007-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Collective excitations in dynamics of liquids: a «toy» dynamical model for binary mixtures</title>
<link href="http://dspace.nbuv.gov.ua:80/handle/123456789/120937" rel="alternate"/>
<author>
<name>Bryk, T.</name>
</author>
<author>
<name>Mryglod, I.M.</name>
</author>
<id>http://dspace.nbuv.gov.ua:80/handle/123456789/120937</id>
<updated>2017-06-14T00:06:37Z</updated>
<published>2007-01-01T00:00:00Z</published>
<summary type="text">Collective excitations in dynamics of liquids: a «toy» dynamical model for binary mixtures
Bryk, T.; Mryglod, I.M.
We propose a new «toy» dynamical model that permits us to derive analytical expressions for dispersion&#13;
of two branches of «bare» propagating collective excitations in binary disordered systems in the whole range&#13;
of wavenumbers. These expressions are used for the analysis of dependence of dispersion curves on mass ratio&#13;
and concentration at fixed density of the system. An effect of hybridization of two branches is discussed&#13;
in terms of mode contributions to time correlation functions. This allows us to estimate the regions with&#13;
dominant types of coherent or partial dynamics.
</summary>
<dc:date>2007-01-01T00:00:00Z</dc:date>
</entry>
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