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Bogolyubov and to the 50th anniversary of the Lviv Department of Statistical Theory of Condensed States of the Bogolyubov Institute of Theoretical Physics, from which the Institute of Condensed Matter Physics was born. A two-day tour to the Carpathians (the Transcarpathian region) will take place after the end of the conference on July 7-8 (Sunday-Monday). The 4th Conference “Statistical Physics: Modern Trends and Applications”, July Lviv, Ukraine (dedicated to the 140th anniversary of the birth of Marian Smoluchowski, whose scientific activity was closely related to the University of Lviv, where he worked since 1899 and held the chair of theoretical physics in 1903-1913).

The purpose of the III CONIN workshop is to summarize recent progress in colloidal and amphiphilic self-assembly and in ionic liquids at room temperature, both in bulk and in confinement, as well as in mobile ions in intercalation compounds and on solids. surfaces. An ab-initio molecular dynamics study of the pressure dependence of collective excitations in a liquid Ga-Sb alloy. Classification of the equilibrium state of magnetic media with spin s=3/2 and SU(4) exchange interaction symmetry.

Resummation of ε-Broadening for Copolymer Star Exponents Reveals Order of Phase Transition in Thermal Denaturation of DNA 24. Effect of Bond Distortion in the Ising-Heisenberg Model on the Shastry-Sutherland Lattice.

Invited Lectures

Abstracts

Quantum simulation requires three important steps: (1) state preparation; (ii) the evolution of the state in time; and (iii) measuring the quantities of interest. Indeed, the same approach applies to the calculation of the rate constants of activated processes and to the generation of hydrodynamic models (convective motion, relaxation of interfaces). I begin with a discussion of the relationship between sociology and statistical physics and how the former inspired the latter 100 years ago.

I discuss some of the joys and difficulties of bridging the academic cultural divide before returning to safe ground of the Ising model. The specific flat-band physics allows a comprehensive description of the thermodynamic properties of Ba2CoSi2O6Cl2 and the prediction of a finite-temperature order-disorder transition in high magnetic fields [1]. However, its applicability depends on the accuracy and the time and length scales of the simulations.

The application of external fields often causes a significant evolution of the local material structure. Reaction and diffusion can be modeled and the stochastic evolution of the system is determined by rules that take into account the local environment and probabilities.

Contributed Talks

Institute for Condensed Matter Physics at the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: adt@icmp.lviv.ua. Formulated free energy of the system of interacting fluctuons produces a thermodynamic equation of state. Finally, we will address the recent signatures of the delocalized Majorana modes in two-dimensional structures.

We find that zeros of the correlation functions are related to the Lee-Yang zeros of partition function of the system. The zeros of two-time correlation functions and the zeros of partition function of the system are found and analyzed. The accuracy of the results is much higher than that in our previous study [Phys.

In this presentation we will discuss some recent advances and applications of the stress fluctuation formalism. The uncorrelated part of the electric field is taken into account via the Poisson equation. According to the reported importance of the intermediate-spin (IS) excitations in LaCoO3 with cubic structure [1,2], we propose that the experimentally observed ferromagnetism in the strained junction [3,4] arises from the highly fluctuating nature of high-spin (HS) states, which can be viewed as biexcitons.

The structural features show features compatible with the appearance of icosahedral short-range order (ISRO) as well as the development of medium-range order (MRO) upon cooling. The weakening of the inner core is due to the unique diffusion characteristic of the bcc phase. Institute of Mathematics of the National Academy of Sciences of Ukraine, 3 Tereschenkivska Str., 01024 Kyiv, Ukraine, E-mail: rebenko@imath.kiev.ua.

Verkin Institute of Low Temperature Physics and Engineering of the National Academy of Sciences of Ukraine, 47 Nauky Ave., 61103, Kharkiv, Ukraine, E-address: slavin@ilt.kharkov.ua. NASU Institute of Mathematics, 3, Tereshchenkivs’ka Str., 01601, Kyiv-4, Ukraine, E-mail: gerasym@imath.kiev.ua. In addition, we determine the asymptotic behavior of the mean field of the propagation process of the initial correlations.

The results show that nanoparticles form layers, and the number of layers depends on the amount of nanoparticles and their diameter. For the studied systems, the formation of layers demonstrates a strong localization of nanoparticles at the interface.

Posters

Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: baliha@icmp.lviv.ua. Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: ost@icmp.lviv.ua. Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: viktoria@icmp.lviv.ua.

Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine. Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E–mail: piv@icmp.lviv.ua. Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine.

Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: dubl@icmp.lviv.ua. The corrections of the result [1] for the steady state temperature of the system are obtained. Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: phl@icmp.lviv.ua.

Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E–mail: ista@icmp.lviv.ua;. The latter is based on the geometric reformulation of the (approximate) linearities of the binodal density diameter (the rectilinear diameter law) and the unit compressibility line (the Zeno line). Institute of Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E–mail: lisnyj@icmp.lviv.ua.

Institute for Condensed Matter Physics ved National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: romanr@icmp.lviv.ua. Institute for Condensed Matter Physics ved National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: port@icmp.lviv.ua. Institute for Condensed Matter Physics ved National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: stetsiv@icmp.lviv.ua.

Institute for Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii Str., 79011 Lviv, Ukraine, E-mail: olve@icmp.lviv.ua.

Figure 1: An example of four-sublattice spin configuration on an anisotropic tri- tri-angular lattice
Figure 1: An example of four-sublattice spin configuration on an anisotropic tri- tri-angular lattice

Author Index

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Figure 1: An example of four-sublattice spin configuration on an anisotropic tri- tri-angular lattice
Figure 1: Dye D205: A-donor, B-bridge, C-acceptor

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