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BEGIN:VEVENT
SUMMARY:Molecular dynamics analysis of particle number fluctuations of a f
 irst-order phase transition
DTSTART;VALUE=DATE-TIME:20240117T144000Z
DTEND;VALUE=DATE-TIME:20240117T150000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-270@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Volodymyr Kuznietsov (University of Houston)\nWe stu
 dy the critical point effects on particle number fluctuations both in the 
 crossover ($T > T_{\\rm c}$) and mixed phase ($T \n\nhttps://indico.bitp.k
 iev.ua/event/11/contributions/270/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/270/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Quantum van der Waals theory of nuclear matter with quarkyonic pha
 se
DTSTART;VALUE=DATE-TIME:20240117T142000Z
DTEND;VALUE=DATE-TIME:20240117T144000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-273@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Roman Poberezhnyuk (Bogolyubov Institute for Theoret
 ical Physics of the National Academy of Sciences of Ukraine)\nWe extend th
 e Quantum van der Waals description of isospin symmetric nuclear matter at
  zero temperature to a high baryon density region by incorporating the con
 tinuous transition to quark matter in accordance with the recently propose
 d quarkyonic approach.  The resulting equation of state exhibits the nucle
 ar liquid-gas transition at $n_B \\leq \\rho_0$ and undergoes a transition
  to quarkyonic matter at densities $n_B \\approx 1.5-2 \\rho_0$ that are r
 eachable in intermediate energy heavy-ion collisions. The transition is ac
 companied by a peak in the sound velocity. The results depend only mildly 
 on the chosen excluded volume mechanism but do require the introduction of
  an infrared regulator $\\Lambda$ to avoid an acausal sound velocity. We a
 lso consider the recently proposed baryquark matter scenario for the reali
 zation of the Pauli exclusion principle\, which yields a similar equation 
 of state and turns out to be energetically favored in all the considered s
 etups.\n\nhttps://indico.bitp.kiev.ua/event/11/contributions/273/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/273/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Constraints on the parameters of the neutrino extension of the Sta
 ndard Model
DTSTART;VALUE=DATE-TIME:20240117T140000Z
DTEND;VALUE=DATE-TIME:20240117T142000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-272@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleksandr Khasai (Bogolyubov Institute for Theoretic
 al Physics of the National Academy of Sciences of Ukraine)\nThis work exam
 ines limitations on the neutrino extension parameters of the Standard Mode
 l of elementary particle physics. A simple relationship between the observ
 ed quantities\, elements of the matrices S and R was obtained\, which is v
 alid for non-zero masses of active neutrinos and for different values of m
 asses of heavy sterile neutrinos. Experimental constraints on the elements
  of the S and R matrices were improved\,  and constraints on $U_{tot}^2$ d
 epending on the mass of a heavy neutrino with right chirality were obtaine
 d.  The expression for the baryon asymmetry of the early Universe also was
  analyzed.\n\nhttps://indico.bitp.kiev.ua/event/11/contributions/272/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/272/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Contribution of one-loop corrections in the decoupling limit of ge
 neralized Yukawa model
DTSTART;VALUE=DATE-TIME:20240117T134000Z
DTEND;VALUE=DATE-TIME:20240117T140000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-283@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Mykyta Dmytriiev (Oles Honchar Dnipro National Unive
 rsity)\nThere exist many models of physics beyond the Standard model (SM) 
 which introduce new heavy particles. Signals of such new states could be p
 arametrized either within a complete model of new physics or its low-energ
 y approximation. The latter consists of effective Lagrangian (EL)\, which 
 describes effects of interactions with heavy particles on the dynamics of 
 light fields when heavy states decouple. Parameters of this EL should be c
 onstrained in experimental data analysis. These constraints\, in turn\, ar
 e translated into limits on parameters of a corresponding complete model. 
 This approach is employed in many researches. In our investigation we show
  that the EL considered in this treatment is valid only if loop correction
 s coming from the light sector of a corresponding complete model are negli
 gible in the decoupling limit.\n	\nOur research is conducted for two scatt
 ering processes which take place in $s$- and $t$-channel\, respectively. T
 ransformational properties of fields and complex interactions within the S
 M are inessential for our analyzis. Hence\, we consider generalized Yukawa
  model instead of a complete SM extended with some new states. We begin wi
 th the following Lagrangian of a complete model:\n\n$$\\begin{equation}\n 
    \\mathcal{L} = \\frac{1}{2}\\left(\\partial_{\\mu}\\phi\\right)^2 - \\f
 rac{1}{2}\\mu^2\\phi^2 + \\frac{1}{2}\\left(\\partial_{\\mu}\\chi\\right)^
 2 - \\frac{1}{2}\\Lambda^2\\chi^2 - \\lambda\\phi^4 - \\rho\\phi^2\\chi^2 
 - \\xi\\chi^4 +\n\\\\ +\\sum\\limits_{a=1\;2}\\bar{\\psi}_a\\left(i\\hat{\
 \partial} - m_a - g_{\\phi}\\phi - g_{\\chi}\\chi\\right)\\psi_a\n\\end{eq
 uation}.~~ (1)$$\n\nThis model consists of two scalar fields $\\phi$ and $
 \\chi$ and two fermionic fields $\\psi_1$ and $\\psi_2$. We put $\\chi$ bo
 son to be much heavier than the other particles of the model\, so $\\Lambd
 a\\gg \\mu\;\\\,m_1\;\\\,m_2$. We derived the following low-energy EL for 
 this model in the limit when $\\chi$ boson decouples:\n\n$$\\begin{equatio
 n}\n    \\mathcal{L}_{eff} = \\frac{1}{2}\\left(\\partial_{\\mu}\\phi\\rig
 ht)^2 - \\frac{1}{2}\\mu^2\\phi^2 - \\lambda\\phi^4 + \\sum\\limits_{a=1\;
 2}\\bar{\\psi}_a\\left(i\\hat{\\partial} - m_a - g_{\\phi}\\phi\\right)\\p
 si_a + \\frac{g_{\\chi}^2}{2\\Lambda^2}\\left(\\bar{\\psi}_1\\psi_1 + \\ba
 r{\\psi}_2\\psi_2\\right)^2.\n\\end{equation}~ (2)$$\n\nHere the last term
  describes effective four-fermion interactions which approximate contribut
 ions of the heavy scalar in observables when $\\chi$ decouples. The other 
 terms in (2) describe dynamics of the model light sector if $g_{\\chi} = 0
 $.\n	\nTwo scattering processes were considered within the complete model 
 (1) and EFT (2) - these are $\\psi_1\\bar{\\psi_1} \\rightarrow \\psi_2\\b
 ar{\\psi_2}$ and $\\psi_1\\psi_2 \\rightarrow \\psi_1\\psi_2$. Cross-secti
 ons of these processes were derived within the complete model (1) in the i
 mproved Born approximation and within the EFT (2). Contributions of radiat
 ive corrections into the cross-sections of these processes were estimated 
 in the decoupling limit. We investigated scenarios where $\\chi$ boson has
  a mass in the interval $20\\mu \\leq \\Lambda \\leq 200\\mu$.\n\n\n(a) Lo
 op corrections to the $\\phi$ boson mass\n\n (b) Diagram of one-loop mixin
 g of light and heavy scalars of\nthe model\n\nFIG. 1: One-loop diagrams wh
 ich become significant at low energies for some values of the model coupli
 ng.\n	\n$~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~$       \nWe found out th
 at if $|g_{\\phi}|$ and $|g_{\\chi}|$ are small\, then the loop correction
 s are negligible and the EL (2) is applicable for description of the scatt
 ering processes at low energies. For the values of $m_1$\, $m_2$ and $\\mu
 $ chosen in our research this takes place if $|g_{\\phi}|  2.5$ then corre
 ctions displayed in Fig.(1a) have a magnitude of more than $10\\\,\\%$ of 
 the $\\chi$ boson mass. These corrections suppress the contribution of the
  heavy scalar in a reaction cross-section. Hence\, if $|g_{\\chi}|$ is big
 \, then (2) significantly overestimates $\\chi$ boson contribution in a cr
 oss-section when $\\chi$ decouples.\n	\nIf $|g_{\\phi}|$ is not small\, th
 en contribution of the scalar fields one-loop mixing is significant in bot
 h $s$- and $t$-channels. One-loop mixing of $\\phi$ and $\\chi$ is introdu
 ced by the diagram in Fig.(1b). In our model\, we get that if $|g_{\\phi}|
  > 1.5$\, then modulus of the contribution of scalars one-loop mixing in t
 he matrix elements of the considered reactions is bigger than $50\\\,\\%$ 
 of the four-fermion interaction term modulus at $s > \\mu^2$ and $|t| > \\
 mu^2$. This was observed in the limit when loop correction in Fig.(1a) is 
 negligible.\n	\nTo conclude\, in our research we have derived the conditio
 ns when radiative corrections to interactions with the heavy boson are neg
 ligible in the decoupling limit in cross-sections of reactions within the 
 generalized Yukawa model. According to these conditions\, radiative correc
 tions become significant if the interactions between light fermions and ei
 ther light or decoupled scalar are not feeble. In such scenarios\, express
 ion (2) should not be used as the low-energy approximation of the model (1
 ). The results obtained in this investigation could be applied to some mod
 els of new physics which extend the SM\, such as the two-Higgs-doublet mod
 el (2HDM). The latter has a limit when new heavy particles decouple. So\, 
 low-energy EL exists for it. Contributions of radiative corrections into c
 ross-sections within the 2HDM should be estimated in the limit when heavy 
 fields beyond the SM decouple. This is the problem left for the future.\n\
 nhttps://indico.bitp.kiev.ua/event/11/contributions/283/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/283/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Searches for axions in proton-proton and ion-ion collisions at ene
 rgies of 5.02 TEV and 13 TEV
DTSTART;VALUE=DATE-TIME:20240117T130000Z
DTEND;VALUE=DATE-TIME:20240117T132000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-276@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Serhii Chernyshenko (Institute for Nuclear Research 
 NAS of Ukraine)\nAs a part of the ATLAS Collaboration experimental measure
 ments of light-by-light\nscattering in Pb+Pb collisions during 2015 and 20
 18 at an integrated luminosity of 2.2 nb-1 and energy of 5.02 TeV\, taking
  into account the obtained experimental constraints [1]\, we have modeled 
 the production cross sections of axion production\, which is candidate for
  dark matter with subsequent decay into γγ. Candidates for light-by-ligh
 t scattering are selected in events with\ntwo photons\, pseudorapidity\, |
 ηγ | \n\nhttps://indico.bitp.kiev.ua/event/11/contributions/276/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/276/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Dynamic Picture of Relativistic Heavy-Ion Collisions
DTSTART;VALUE=DATE-TIME:20240117T124000Z
DTEND;VALUE=DATE-TIME:20240117T130000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-290@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Musfer Adzhymambetov (Bogolyubov Institute for Theor
 etical Physics of the National Academy of Sciences of Ukraine)\nCollider e
 xperiments serve as an unique tool to create and study new forms of strong
 ly interacting matter\, such as quark-gluon plasma (QGP). This state of ma
 tter is believed to have existed in the microseconds after the Big Bang wh
 en temperatures and energy densities were extremely high. However\, due to
  confinement under typical Earth conditions\, elementary particles of quan
 tum chromodynamics (QCD) exist only in colorless combinations within hadro
 ns. Lattice QCD calculations show that at zero chemical potential\, there 
 is no phase transition between these two states of matter - QGP and hadron
  gas. However\, in baryon-rich regions of the QCD phase diagram\, a phase 
 transition of finite order is expected to occur which ends with a critical
  point.\nOne of the primary goals of current and future experimental progr
 ams\, including RHIC BES and CBM\, is to search for the signal of the crit
 ical point in observables. Such studies demand a comparison with predictio
 ns of theoretical models. In this talk\, I will present a recently develop
 ed integrated Hydro-Kinetic model tailored to describe the full dynamics o
 f the system created in heavy-ion collisions at relatively low energies. A
 dditionally\, I will discuss an idea for searching for signals of the crit
 ical point through a comparison of model simulations and experimental data
 .\n\nhttps://indico.bitp.kiev.ua/event/11/contributions/290/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/290/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Bremsstrahlung emission in proton-deuteron scattering and nucleon-
 nucleon forces
DTSTART;VALUE=DATE-TIME:20240117T122000Z
DTEND;VALUE=DATE-TIME:20240117T124000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-271@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Kostiantyn Shaulskyi (Institute for Nuclear Research
 )\nWe will present the results of a study of the bremsstrahlung emission o
 f photons in a process of proton scattering on deuterons. Despite the long
  history of studies of the interaction of protons with deuterons and the e
 xistence of some studies on the subject in such reactions there are some i
 nteracting problems that need to be tackled. This stimulates us to develop
  a new model that allows us to gain more information about processes induc
 ed by the $p + d$ interaction and the properties of nuclear forces. Beside
 s\, this model is aimed at detailed analysis and interpretation of the exi
 sting experimental data on bremsstrahlung emission in these processes. The
  relative simplicity of the selected nuclei is explained by the fact that 
 it is possible to demonstrate more clearly the effectiveness of the model.
 \n\nThe quantum model of photon emission developed by us is a continuation
  of the development of methods of bremsstrahlung emission in nuclear proce
 sses formulated in [1\, 2] (see references therein) with new incorporating
  ideas of cluster models [3\, 4] (see references therein). Within the fram
 ework of the model\, proton scattering on a deuteron is described as a sol
 ution of the quantum-mechanical three-nucleon problem with semi-realistic 
 nucleon-nucleon potentials. This model is applied to study wave functions 
 of continuous spectrum states in the $p + d$ system and then to calculate 
 cross sections of photon emission. Based on this model\, a good descriptio
 n of the existing experimental emission data has been achieved [5\, 6]. Th
 e dependence of the cross sections of bremsstrahlung emission on the shape
  of the nucleon-nucleon potential is studied in details.\n\nWe have applie
 d our method to analyse results of experimental investigations [5\, 6] of 
 gamma ray production in $p + d$ interactions. Our analysis revealed that t
 he results of the experiments [5\, 6] with chosen parameters (incident ene
 rgy of proton beam\, energy of detected photons) are insensitive to the pe
 culiarities of nuclear forces. However\, we have identified another energy
  region for experiments where it is possible to obtain information about t
 he properties of nuclear forces within the present method with higher accu
 racy. To make our analysis more complete\, we analyze bremsstrahlung prope
 rties in a wide range of proton beam energies and photon energies.\n\nResu
 lts of our model allow us to predict behavior of bremsstrahlung cross sect
 ions which can be used for planning of new experiments. The approach devel
 oped can be used to study the bremsstrahlung emission in a large variety o
 f nuclear scattering processes\, and also to determine effects of nuclear 
 structure and nucleusnucleus interaction on a such emission.\n\n1. S.P. Ma
 ydanyuk. Enhancement of incoherent bremsstrahlung in proton-nucleus scatte
 ring in the ∆-\nresonance energy region. Phys. Rev. C107\, 024618 (2023)
 \, arXiv: 2203.07146.\n2. X. Liu et al. First investigations of hypernucle
 i in reactions via analysis of bremsstrahlung photons. Phys. Rev. C99\, 06
 4614 (2019)\, arXiv: 1810.11942.\n3. V. Vasilevsky et al. Algebraic model 
 for scattering in three s cluster systems. 1. Theoretical background. Phys
 . Rev. C63\, 034606 (2001).\n\nhttps://indico.bitp.kiev.ua/event/11/contri
 butions/271/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/271/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Nature of Pauli resonances states in light nuclei
DTSTART;VALUE=DATE-TIME:20240117T120000Z
DTEND;VALUE=DATE-TIME:20240117T122000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-282@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Nursultan Kalzhigitov (Al-Farabi Kazakh National Uni
 versity)\nThe resonating group method (RGM) [1] is a rigorous and self-con
 sistent realization of cluster model. It has been numerously proved the RG
 M is a powerful tool to study the structure of light atomic nuclei and nuc
 lear reactions of different types. Thus it equally well describes bound an
 d continuous spectrum states. The main advantages of the RGM is that it ta
 kes into account the internal structure of interacting nuclei (clusters) a
 nd correctly treats the Pauli principle. In the standard (initial) version
  of the RGM\, the internal structure of clusters was described by wave fun
 ctions of the many-particle shell model. Then\, many attempts have been ma
 de (undertaken) to use more realistic wave functions of clusters. They aim
 ed at a more correct description of interacting clusters and compound syst
 em as well. These attempts brought new interesting results. However\, they
  also gave a birth of a new problem\, which is called the Pauli resonances
  and which are considered as a redundant solutions of the RGM equations. I
 t was recognized\, the Pauli principle is the origin of the problem.\nIn o
 ur work\, we perform a systematic investigation of the Pauli resonance sta
 tes in the continuum spectrum of light atomic nuclei: $^6$Li\, $^7$Li\, $^
 8$Be\, $^9$Be and $^{10}$B. These nuclei are considered as two-cluster sys
 tems. One of the clusters of two-cluster system\, which is weakly bound\, 
 is also considered as a two-cluster system. We especially interested in th
 e Pauli resonance states appearing in interaction of neutrons\, protons\, 
 deuteron\, tritons and alpha particles with $^6$Li. For this purpose\, we 
 employ of a microscopic three-cluster model\, formulated in [2]. This mode
 l uses square-integrable Gaussian and oscillator bases to expand wave func
 tion of relative motion of clusters. As a result\, the many-particle Schr
 ödinger equation is transformed into a set linear algebraic equations. It
  is numerously demonstrated that discrete algebraic form of two-cluster Ha
 miltonian is the best way to analyze effects of the Pauli principle.\nIt i
 s shown that the Pauli resonance states in selected nuclei lie in the ener
 gy range between 11 and 45 MeV\, and their widths are varied from 8 keV to
  8 MeV.  It is demonstrated that in main cases\, only one Pauli resonance 
 emerges in continuous spectrum of two-cluster systems. We have also found 
 several cases when two Pauli resonances are formed by interaction of two c
 lusters.\nAnalysis of wave functions of the Pauli resonance states and the
  many-particle Schrödinger equation in the discrete space allowed us to f
 ormulate an algorithm for elimination of Pauli resonance states. This algo
 rithm suggests new definition of so-called totally-forbidden and almost-fo
 rbidden Pauli states which are responsible for creation of the Pauli reson
 ances. It is demonstrated that the suggested algorithm completely eliminat
 es all Pauli resonance states.\n\n1. J.A. Wheeler\, Phys. Rev. 52\, 1107 (
 1937).\n2. V.S. Vasilevsky\, F. Arickx\, et al.  Nucl. Phys. A. 824\, 37 (
 2009).\n\nhttps://indico.bitp.kiev.ua/event/11/contributions/282/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/282/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Influence of the variable cross section on the domain wall dynamic
 s in curved ferromagnetic nanostripes
DTSTART;VALUE=DATE-TIME:20240117T105000Z
DTEND;VALUE=DATE-TIME:20240117T111000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-266@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Dmytro Karakuts (Taras Shevchenko National Universit
 y of Kyiv\, 01601 Kyiv\, Ukraine)\nCurvilinear magnetism is an emerging fi
 eld which connects low-dimensional magnetic architectures with their geome
 trical properties to describe resulting novel phenomena. Nanoscale curved 
 magnetic stripes are a crucial building block in the race for high-density
  and ultrafast magnetic memory\, and can substantially augment the perform
 ance of spintronic devices [1\,2].\n\nHere\, we aim to theoretically and n
 umerically study how changes in the cross-section area of the curved ferro
 magnetic nanostripe affect its magnetic structure. Namely\, we show that t
 ailoring of the gradient of the cross-section area can be used to control 
 the motion of the domain wall. Although\, the magnetic response of the cur
 ved nanostripe is already well-studied\, in all previous studies cross sec
 tion of the nanowire was assumed to be constant. Only recently\, a new mic
 romagnetic framework emerged that allows the exploration of the changes in
  the magnetization dynamics caused by the cross-section area gradient [3].
 \n\nHere\, we use the collective variable approach by adapting the q-Ф mo
 del to stripes with varying cross section. The description of the domain w
 all motion in ferromagnetic wires is investigated by considering the tempo
 ral evolution of the magnetization vector based on the Landau–Lifshitz
 –Gilbert equation. To derive the specific equations of motion for the co
 llective variables\, the Lagrange-Rayleight formalism is used\, where the 
 dependency on the spatial variation of the cross-section area is factored 
 in both the Lagrangian and the dissipative function.\n\nThe resulting equa
 tions of the domain wall motion are studied for three specific geometries:
  a straight stripe\, an arc of a circle and an Euler spiral. For the case 
 of a straight stripe with absent curvature\, we show that the domain wall 
 velocity is mainly determined by the cross-section gradient. For the case 
 of constant curvature\, the asymptotic domain wall velocity is shown to ha
 ve two components: the first component is identical to the speed of the do
 main wall in the straight wire\, while the second one describes the coupli
 ng between the curvature and the cross-section gradient. For the case of t
 he wire\, whose curvature grows at a constant rate\, the asymptotic domain
  wall velocity has two contributions. The first one is the same as the vel
 ocity in the straight wire\, however\, the second one differs from the pre
 vious case and is determined solely by the rate of curvature growth. All a
 nalytical predictions are well­confirmed by the NMAG micromagnetic simula
 tions [4].\n\nThe gradient of the cross-section area of the curved ferroma
 gnetic nanostripe creates an internal driving force\, which in turn induce
 s the domain wall motion and can explain the recent experimental results [
 5]. We have shown how the dynamics of the domain wall motion can be modifi
 ed through tailoring the cross-section area of the nanostripe. Although we
  showcased our approach only for three specific geometries\, it is general
  and can be applied to a wide class of geometries.\n\n1. Curvilinear Micro
 magnetism: From Fundamentals to Applications\, edited by D. Makarov and D.
  Sheka\, Topics in Applied Physics Vol. 146 (Springer\, Cham\, 2022).\n2. 
 D. D. Sheka\, O. V. Pylypovskyi\, O. M. Volkov\, K. V. Yershov\, V. P. Kra
 vchuk\, and D. Makarov\, Small 18\, 2105219 (2022).\n3.	K. V. Yershov\, D.
  D. Sheka\, Phys. Rev. B 107\, L100415 (2023).\n4. T. Fischbacher\, M. Fra
 nchin\, G. Bordignon and H. Fangohr\, IEEE Transactions on Magnetics\, Vol
 . 43\, No. 6\, (2007).\n5. L. Skoric et al. ACS Nano 16\, 8860 (2022).\n\n
 https://indico.bitp.kiev.ua/event/11/contributions/266/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/266/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Nonlinear wave phenomena in Josephson junctions
DTSTART;VALUE=DATE-TIME:20240117T100500Z
DTEND;VALUE=DATE-TIME:20240117T105000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-287@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Yaroslav Zolotaryuk (Bogolyubov Institute for Theore
 tical Physics of the National Academy of Sciences of Ukraine)\nhttps://ind
 ico.bitp.kiev.ua/event/11/contributions/287/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/287/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Spatial coherence of compact sources with respect to X-ray phase c
 ontrast imaging formation
DTSTART;VALUE=DATE-TIME:20240117T092500Z
DTEND;VALUE=DATE-TIME:20240117T094500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-277@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Artur Ovcharenko (Institute of Applied Physics of th
 e NAS of Ukraine)\nSignificant successes and important results of research
  on synchrotron radiation sources raised a new urgent question\, namely th
 e development of bright compact radiation sources with coherence parameter
 s that allow the implementation of phase-informative methods. This is due 
 to the growing demand for the use of new research methods based on X-ray r
 adiation in engineering\, materials science and medicine. The study concer
 ns the topical issue of implementation of diffraction research methods on 
 compact radiation sources [1]. Taking into account phase information helps
  to increase the sensitivity and informativeness of the obtained images\, 
 making their use more effective in a wide range of research and diagnostic
  tasks.\n\nThe aim is to determine the research capabilities of various ty
 pes of installations in solving specific applied problems\, as well as to 
 develop applied calculation methods for planning and conducting X-ray phas
 e contrast experiments. X-ray phase contrast arises due to the difference 
 in the phase of X-rays when they pass through objects with different refra
 ctive or absorption indices. One of the approaches for modeling X-ray phas
 e contrast is the Fresnel-Kirchhoff scalar diffraction theory [2-4]. This 
 study presents a method for calculating phase-contrast images of test obje
 cts. A two-stage algorithm for calculating the X-ray phase contrast image 
 from sources of different shapes and sizes has been developed. The evoluti
 on of the wave front along the source-object and object-screen path is tak
 en into account. The source-object and object-screen distances at which it
  is possible to observe phase-contrast images in the Fresnel region have b
 een found. Simulated images of test objects were obtained in the form of i
 ntensity contrast on the screen and its phase profile. As the calculations
  show\, increasing the thickness of certain sections of the test object le
 ads to changes in the phase distribution and intensity of the resulting im
 age. This is manifested in the form of the appearance of intensity maxima 
 at the edges of the object\, where there is a fast change in its thickness
 \, as well as minima\, where the thickness is the largest\, which is expla
 ined by a greater deviation of X-rays from their original direction.\n\nTh
 e results of the research will be useful for the development of methods fo
 r studying the internal structure of materials\, as well as for solving pr
 oblems in medical diagnostics\, where X-ray phase contrast can help distin
 guish tissues with different physical properties\, for example\, in the st
 udy of soft tissues and organs.\n\n1.	L. Quenot\, S. Bohic and E. Brun\, A
 ppl. Sci.\, 12(19)\, 9539\; (2022)\nhttps://doi.org/10.3390/app12199539\n2
 .	D. Paganin Coherent x-ray optics. Oxford University Press\, 2013\, 424 p
 p.\n3.	V. Kolobrodov\, G. Timchyk\, Applied Diffraction Optics: Textbook\,
  K.: NTUU "KPI"\, 2014\, 312 pp.\n4.	A. Pil-Ali et al.\, Proc. SPIE 11595\
 , Medical Imaging 2021: Physics of Medical Imaging\, 115951N (15 February 
 2021)\; doi: 10.1117/12.2582225\n\nhttps://indico.bitp.kiev.ua/event/11/co
 ntributions/277/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/277/
END:VEVENT
BEGIN:VEVENT
SUMMARY:The Mutual Influence of Production Rate of Point Defects and Tempe
 rature on the Effects of Radiation-Induced Segregation in the Fe-20Cr-8Ni 
 Alloy
DTSTART;VALUE=DATE-TIME:20240117T090500Z
DTEND;VALUE=DATE-TIME:20240117T092500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-274@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Roman Skorokhod (Institute of Applied Physics of Nat
 ional Academy of Sciences of Ukraine\, Sumy\, Ukraine)\nIn this paper\, a 
 computer simulation of radiation-induced segregation in the Fe-20Cr-8Ni al
 loy was carried out within the framework of the modified inverse Kirkendal
 l model [1-3]. The dependences of the concentrations of Cr and Ni atoms on
  the surface of the sample on the rate of production of point defects and 
 temperature\, as well as the concentration profiles of Cr and Ni atoms and
  point defects\, were calculated. The influence of the rate of production 
 of point defects and temperature on the concentration profiles of componen
 ts and point defects is analyzed in detail. It is shown that the effect of
  the increase in the rate of production of point defects on the concentrat
 ion profiles of the alloy components can be compensated with a sufficientl
 y high accuracy by a relatively small increase in temperature (fig. 1). Th
 is effect is explained by the competition of two mechanisms: (i) increasin
 g the irradiation of the alloy leads to a narrowing of the concentration p
 rofiles\; (ii) an increase in temperature leads to a broadening of concent
 ration profiles.\n\nFig. 1. Concentration profiles of Cr and Ni in the Fe-
 20Cr-8Ni alloy under irradiation.\n\n1. G.S. Was\, *Fundamentals of Radiat
 ion Materials Science. Metals and Alloys* (2nd ed.) (New York: Springer: 2
 017).\n2. R.V. Skorokhod\, O.M. Buhay\, V.M. Bilyk\, V.L. Denysenko and O.
 V. Koropov\, *East European Journal of Physics*\, **5**\, No. 1: 61–69 (
 2018) (in Ukrainian).\n3. R.V. Skorokhod and O.V. Koropov\, *Metallofiz. N
 oveishie Tekhnol.*\, **44**\, No. 6: 691—711 (2022) (in Ukrainian).\n\nh
 ttps://indico.bitp.kiev.ua/event/11/contributions/274/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/274/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Revealing inaccuracies of the GFN1-xTB semi-empirical method with 
 machine-learning toolset
DTSTART;VALUE=DATE-TIME:20240117T084500Z
DTEND;VALUE=DATE-TIME:20240117T090500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-275@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Andrii Terets (1) Faculty of Physics\, Taras Shevche
 nko National University of Kyiv. 2)  Chuiko Institute of Surface Chemistry
 \, NAS of Ukraine\,)\nThe change in conformation during biological functio
 ning is a characteristic feature of biomolecules. The presence of various 
 conformers complicates their physics-based modeling\, as the properties of
  each conformer need to be determined separately. Moreover\, the relative 
 energies of the conformers become an additional quantity of interest becau
 se they determine the probability of each conformation in a real system.\n
 \nAlthough ab initio quantum-mechanical methods are the most accurate for 
 determining the physical properties of molecules\, their computational cos
 ts become prohibitive when applied to biomolecules with a large number of 
 atoms and/or a large number of conformations. Semi-empirical quantum mecha
 nical methods\, particularly those based on the tight-binding approximatio
 n in density functional theory (DFTB)\, significantly reduce computational
  requirements by utilizing parameterized models for the elements of the Fo
 ck or Kohn-Sham matrices. However\, due to such simplifications\, the resu
 lting method can show low accuracy in some cases\, despite performing accu
 rately in other cases.\n\nIn this work\, we demonstrate that machine learn
 ing (ML) methods such as graph neural networks and ensemble models can be 
 employed to predict errors in determining the relative energies of conform
 ers by the semi-empirical method GFN1-xTB from the DFTB family\, based sol
 ely on the molecular structural formula as input.\n\nThe developed ML ense
 mble model achieves an accuracy of about 80% in determining whether a give
 n molecule is 'challenging' for GFN1-xTB. This approach can be used to fin
 d the molecules that most vividly highlight the shortcomings of the physic
 al model underlying the GFN1-xTB method. We demonstrate that for the 190 m
 olecules selected using the developed model\, the average error in relativ
 e energies of their conformers obtained by the GFN1-xTB method is 4.2 kcal
 /mol\, in contrast to 1.8 kcal/mol when the same number of test molecules 
 are selected randomly. This indicates that the ML toolset indeed allows fo
 r the identification of challenging molecules and can therefore be useful 
 in improving the approximations utilized by semi-empirical methods.\n\nhtt
 ps://indico.bitp.kiev.ua/event/11/contributions/275/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/275/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Application of machine learning approaches to the generation of or
 ganic compounds and prediction of their properties
DTSTART;VALUE=DATE-TIME:20240117T080000Z
DTEND;VALUE=DATE-TIME:20240117T084500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-288@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Maksym Druchok (Institute for Condensed Matter Physi
 cs of the National Academy of Sciences of Ukraine)\nhttps://indico.bitp.ki
 ev.ua/event/11/contributions/288/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/288/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Perturbation equations for Schwarzschild geodesics
DTSTART;VALUE=DATE-TIME:20240116T144500Z
DTEND;VALUE=DATE-TIME:20240116T150500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-268@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleksii Yanchyshen (Bogolyubov Institute for Theoret
 ical Physics)\nIn our work we consider geodesic equations in Schwarzschild
  space-time with arbitrary external forces and obtain Gaussian perturbatio
 n equations for osculating elements in terms of Weierstrass elliptic funct
 ions. As an application\, we solve the perturbation equations analytically
  in linear approximation for forces induced by the presence of the cosmolo
 gical constant in the Schwarzschild-de Sitter metric\, which we compared w
 ith a known analytical solution. Also\, we solve the perturbation equation
 s for hybrid Schwarzschild/post-Newtonian $2.5$ order self-forces.\n\nhttp
 s://indico.bitp.kiev.ua/event/11/contributions/268/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/268/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Long-time asymptotic series for the Painleve II equation: Riemann-
 Hilbert approach
DTSTART;VALUE=DATE-TIME:20240116T142500Z
DTEND;VALUE=DATE-TIME:20240116T144500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-267@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Yurii Zhuravlov (Bogolyubov Institute for Theoretica
 l Physics of the National Academy of Sciences of Ukraine)\nWe elaborate a 
 systematic way to obtain higher order contributions in the nonlinear steep
 est descent method for Riemann-Hilbert problem associated with homogeneous
  Painleve II equation. The problem is reformulated as a matrix factorizati
 on problem on two circles and can be solved perturbatively reducing it to 
 finite systems of algebraic linear equations. The method is applied to fin
 d explicitly long-time asymptotic behaviour for tau function of Painleve I
 I equation.\n\nhttps://indico.bitp.kiev.ua/event/11/contributions/267/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/267/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Andreev reflection in scanning tunneling spectroscopy of unconvent
 ional superconductors
DTSTART;VALUE=DATE-TIME:20240116T140500Z
DTEND;VALUE=DATE-TIME:20240116T142500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-263@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Pavlo Sukhachov (University of California\, Santa Cr
 uz)\nMotivated by recent experimental observations of unconventional super
 conductivity in the twisted bilayer and trilayer graphene\, we develop a t
 heory of point-contact tunneling into superconductors with arbitrary gap s
 tructures and for arbitrary transmission coefficients of the contact. Expl
 oiting the dependence of Andreev reflections on the position of the STM ti
 p relative to lattice symmetry points\, we show that the nature of the ord
 er parameter can be extracted by combining weak- and strong-tunneling limi
 ts of differential conductance. This provides complementary information ab
 out the superconducting gap structure beyond the tunneling density of stat
 es\, strongly facilitating the ability to extract the gap symmetry and its
  relation to the underlying crystalline lattice. We use the developed theo
 ry to discuss recent experimental results on superconductivity in twisted 
 bilayer graphene.\n\nhttps://indico.bitp.kiev.ua/event/11/contributions/26
 3/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/263/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Theory of low-frequency electron fluctuations in a quasi-ballistic
  FET
DTSTART;VALUE=DATE-TIME:20240116T132500Z
DTEND;VALUE=DATE-TIME:20240116T134500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-264@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Mykola Yelisieiev (Institute of Semiconductor Physic
 s\, NAS of Ukraine\, Kyiv\, Ukraine)\nWe investigated the electronic proce
 sses in a field effect transistor channel using shallow water approximatio
 ns to obtain the analytical expressions for electron and field distributio
 ns\, as well as electric fluctuations using the Langevin approach. We cons
 idered the current-voltage characteristic of the transistor in the station
 ary mode. For the non-stationary case\, we obtained the spatial distributi
 ons of the spectral fluctuations density for different parameters of the c
 hannel\, and the dependence of these values on the stationary parameters. 
 We considered two modes of measuring transistor characteristics with a fix
 ed voltage  or current.\n\nhttps://indico.bitp.kiev.ua/event/11/contributi
 ons/264/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/264/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Optimization of quantum logic gates based on nonadiabatic Landau-Z
 ener-Stückelberg-Majorana transitions
DTSTART;VALUE=DATE-TIME:20240116T130500Z
DTEND;VALUE=DATE-TIME:20240116T132500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-278@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleh Ivakhnenko (B. Verkin ILTPE of NASU | RIKEN\, J
 apan)\nQuantum logic gates applied to qubits are basic elements of the cir
 cuit model used for quantum computations. Usually\, quantum gates are real
 ized by a resonant excitation\, resulting in Rabi oscillations\, which lea
 d to a periodic excitation of the qubit. It has certain limitations and co
 mplications\, like neglecting counter-rotating terms. We investigate an al
 ternative way for quantum control and performing of quantum logic gates wi
 th Landau-Zener-Stückelberg-Majorana (LZSM) transitions [1\,2\,3] using n
 onadiabatic driving and alternation of the two stages of evolution: adiaba
 tic evolution and non-adiabatic transitions. We investigate mechanisms\, d
 ynamics\, and ways to optimize single-qubit LZSM gates [1\,3]. We apply th
 e adiabatic-impulse model to describe multiple LZSM transitions [1\,3]\, w
 hich we use to create LZSM-based quantum logic gates. Any single-qubit ope
 ration can be realized with only two LZSM transitions with an adjustable t
 ime of free evolution time before and after those transitions. To gain bet
 ter fidelity and reduce quantum gates performing time\, we can use multipl
 e LZSM transitions. LZSM-based quantum logic gates in comparison with Rabi
  oscillations based gates allow us to reduce gate time with keeping fideli
 ty high\, enabling us to perform more gates before the impact from decoher
 ence and relaxation becomes significant. Fig.1 shows the dynamics for the 
 NOT (X) gate realized by double LZSM transitions.\nAcknowledgments: This r
 esearch was funded by the Army Research Office and was supported by Grant 
 No. 911NF-20-1-0261\, RIKEN International Program Associate.\n\n1. A. Ryzh
 ov\, O. Ivakhnenko\, S. Shevchenko\, «Alternative fast quantum logic gate
 s using nonadiabatic Landau-Zener-Stückelberg-Majorana transitions»\, Ar
 Xiv:2310.17932\, 2023 \n2. D. Campbell\, et al.\, «Universal nonadiabatic
  control of small-gap superconducting qubits»\, Phys. Rev. X\, 2020 10\, 
 041051 \n3. O. V. Ivakhnenko\, S. N. Shevchenko and F. Nori «Nonadiabatic
  Landau-Zener-Stückelberg-Majorana transitions\, dynamics\, and interfere
 nce»\, Phys. Rep.\, 2023\, 995\, 1.\n\n\nFig. 1. Dynamics for the NOT (X)
  gate with ground initial state with double LZSM transitions: (a) dynamics
  on the Bloch sphere\, (b) dynamics of Bloch coordinates.\n\nhttps://indic
 o.bitp.kiev.ua/event/11/contributions/278/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/278/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Theoretical study of a transmon-type qubit connected to a semi-inf
 inite transmission line
DTSTART;VALUE=DATE-TIME:20240116T124500Z
DTEND;VALUE=DATE-TIME:20240116T130500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-284@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Maksym Liul (B. Verkin ILTPE of NASU)\nThe research 
 is dedicated to a detailed theoretical study of dynamic processes that occ
 ur during the interaction of a transmon-type qubit connected to a semi-inf
 inite transmission line with two signals: pump and probe. By manipulating 
 the frequencies and amplitudes of the signals it is possible to explore th
 e system behavior. We use the Lindblad equation formalism to make our calc
 ulations. From the solution of the Lindblad equation one can get upper cha
 rge level occupation probability as a function of pump and probe signals p
 arameters (amplitudes and frequencies) and build these dependencies. \nIn 
 Ref. [1] the authors mentioned that the experimentally measured reflection
  coefficient corresponds to upper charge level occupation probability in t
 he theory. In Ref. [2] the theoretical model describing the system was dev
 eloped and approved experimentally. The current research is an extension o
 f the corresponding article: here we build the dependencies which were not
  considered before. Particularly we studied the steady state\, by plotting
  the dependence of upper charge level occupation probability on the probe 
 frequency and the pump frequency. For studying dynamics the upper charge l
 evel occupation probability was built as a function of (a) time and the pr
 obe frequency\; (b) time and the probe frequency. The obtained plots provi
 de a deeper insight into the underlying physical processes and could be va
 luable for guiding future experiments. Additionally\, we address the Lindb
 lad equation using Lindblad superoperators in different bases. In our opin
 ion\, this comparative analysis holds significant methodological importanc
 e.\n\nAcknowledgments\nThe author was partially supported by the grant fro
 m the National Academy of Sciences of Ukraine for research works of young 
 scientists (1/H-2023\, 0123U103073).\n\n1. P. Y. Wen\, O. V. Ivakhnenko\, 
 M. A. Nakonechnyi\, B. Suri\, J.-J. Lin\, W.-J. Lin\, J. C. Chen\, S. N. S
 hevchenko\, F. Nori\, and I.-C. Hoi\, Landau-Zener-Stückelberg-Majorana i
 nterferometry of a superconducting qubit in front of a mirror\, Phys. Rev.
  B 102\, 075448 (2020).\n2. M. P. Liul\, C.-H. Chien\, C.-Y. Chen\, P. Y. 
 Wen\, J. C. Chen\, Y.-H. Lin\, S. N. Shevchenko\, F. Nori\, and I.-C. Hoi\
 , “Coherent dynamics of a photon-dressed qubit\,” Phys. Rev. B 107\, 1
 95441 (2023).\n\nhttps://indico.bitp.kiev.ua/event/11/contributions/284/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/284/
END:VEVENT
BEGIN:VEVENT
SUMMARY:History and modern trends in thermoelectric and thermomagnetic phe
 nomena
DTSTART;VALUE=DATE-TIME:20240116T120000Z
DTEND;VALUE=DATE-TIME:20240116T124500Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-286@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Sergei Sharapov (Bogolyubov Institute for Theoretica
 l Physics of the National Academy of Sciences of Ukraine)\nhttps://indico.
 bitp.kiev.ua/event/11/contributions/286/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/286/
END:VEVENT
BEGIN:VEVENT
SUMMARY:How partition function zeros help find out the finite-size scaling
  above the upper critical dimension
DTSTART;VALUE=DATE-TIME:20240116T093000Z
DTEND;VALUE=DATE-TIME:20240116T095000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-285@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Yulian Honchar (Institute for Condensed Matter Physi
 cs of the National Academy of Sciences of Ukraine\, Lviv\; Centre for Flui
 ds and Complex Systems\, Coventry University\,Coventry CV1 5FB\, UK\; L4 C
 ollaboration and Doctoral College for the Statistical Physics of Complex S
 ystems\, Lviv-Leipzig-Lorraine-Coventry\, Europe)\nFor many years the ques
 tion of finite-size scaling above the upper critical dimension dc was a so
 urce of many new theoretical results as well as new and interesting works 
 in computer simulations\, see [1] for a review . While in the thermodynami
 c limit system’s scaling behaviour is mean-field\, for the finitesize sy
 stems two scaling regimes are being considered. Simple approach is a trivi
 al renormalization group fixed point\, obtained by setting all fields to z
 ero\, called Gaussian fixed point\, or G-scaling. Second scaling regime in
 troduces a new scaling exponent $q = max(1\, d/d_c)$\, that governs the sc
 aling of correlation length  $\\xi$ with system size L\, it is called Q-sc
 aling. The latter was confirmed for periodic boundary conditions\, both at
  the infinite system’s critical temperature and at the pseudocritical po
 ints. For lattices with free boundary conditions the shifting and rounding
  of the susceptibility peak that occurs at the pseudocritical point are bi
 g enough to position the pseudocriticality far from the critical point of 
 the infinite system. This leads to both scaling regimes emerge\, so theory
  predicted G-scaling at $T_c$ and Q-scaling at $T_L$. Numerical validation
  of the finite-size scaling for free boundary conditions was not clear\, a
 s the boundary effects are too strong to observe the scaling picture accur
 ately. In this work we show the shortcomings of the regular computer simul
 ations methods and improve the quality of the finite-size scaling using th
 e Lee-Yang zeros technique. Using the partition function zeros provides us
  with the more accurate scaling picture with smaller lattice sizes at hand
  [2].\n\n1. Berche\, B.\; Ellis\, T.\; Holovatch\, Yu.\; Kenna\, R. Phase 
 Transitions above\nthe Upper Critical Dimension. SciPost Phys. Lect. Notes
  2022\, 60. DOI:\n10.21468/SciPostPhysLectNotes.60\n2. Honchar Yu.\, Berch
 e B.\, Holovatch Yu.\, Kenna R. When correlations exceed\nsystem size: fin
 ite-size scaling in free boundary conditions above the upper\ncritical dim
 ension. // preprint ArXiv:. - 2023. - arXiv:2311.11721. (to\nappear in Con
 dens.Matter Phys 2024\, 1) DOI:10.48550/arXiv.2311.11721\n\nhttps://indico
 .bitp.kiev.ua/event/11/contributions/285/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/285/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Phase behavior of ionic liquids in disordered porous media
DTSTART;VALUE=DATE-TIME:20240116T080500Z
DTEND;VALUE=DATE-TIME:20240116T085000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-289@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Taras Patsahan (Institute for Condensed Matter Physi
 cs  of the National Academy of Sciences of Ukraine)\nhttps://indico.bitp.k
 iev.ua/event/11/contributions/289/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/289/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Towards the influence of compaction on the compressibility of a mo
 del bi-component mixture
DTSTART;VALUE=DATE-TIME:20240116T091000Z
DTEND;VALUE=DATE-TIME:20240116T093000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-280@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Heorhiy Kudashkin (Odesa State Environmental Univers
 ity)\nThere are well-defined indications\, following from experimental stu
 dies of compressibility (adiabatic compressibility is measured using sound
  speed measurements\, and then isothermal compressibility is restored)\, t
 o the existence of a dependence of the compressibility of simple bi-compon
 ent mixtures not only on the molar fractions of the components [1]. It can
  be assumed that this parameter may be the compaction (packaging) paramete
 r [2].\nIn this way\, this work examines the question of the influence of 
 the packing parameter on the compressibility of a model two-component mixt
 ure. For this purpose\, it is proposed to use extensions of the model equa
 tions of state (for example\, the van der Waals equation is chosen) for th
 e case of a two-component mixture together with an equation for compressib
 ility\, following from the Carnahan-Starling-Mansoori theory [3]\, which o
 perates precisely with the compactization factor.\nAnalytical expressions 
 have been obtained to express the compressibility of a binary mixture thro
 ugh the molar fractions of the components and the compaction of the entire
  bi-component system. Using the obtained analytical expressions\, three-di
 mensional phase diagrams have been constructed in the axes compressibility
 \, the molar fraction of one of the components\, and the compaction of the
  mixture\, allowing one to track the joint influence of these parameters o
 n the equation of state model bi-component system.\nAs a result of studyin
 g the obtained phase diagrams\, it was established that the influence of i
 nternal parameters (molar composition\, compaction) is carried out jointly
  and consistently (multi-parameter). Mole composition and compaction\, for
  model systems (such as the hard ball model) are among the carefully contr
 olled parameters and thus\, the proposed model for describing compressibil
 ity is suitable for use to parameterize the results of empirical studies o
 f the dependence of the compressibility of simple binary mixtures (liquid\
 , or granular) to the theoretical description of which the concept of hard
  spheres is applicable.\n\nREFERENCES\n\n1.	F.  Aliotta et al.\, J. Phys. 
 Chem.\, 2007. 126\, 224508. https://doi.org/10.1063/1.2745292\n2.	O. I. Ge
 rasymov et al.\, Tightening (Compaction) of Bi-Component Micromechanical (
 Granular) System. Sci. innov.\, 2021. V. 17\, no. 4. P. 79—88.\nhttps://
 doi.org/10.15407/scine17.04.079\n3.	G. A. Mansoori\, N. F. Carnahan\, K.E.
  Starling\, T. W. Leland Jr. Equilibrium Thermodynamic Properties of the M
 ixture of Hard Spheres. The Journal of Chemical Physics\, 1971. 54(4)\, 15
 23—1525. https://doi.org/10.1063/1.1675048.\n\nhttps://indico.bitp.kiev.
 ua/event/11/contributions/280/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/280/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Towards the modeling of impurity migration in a heterogeneous medi
 a
DTSTART;VALUE=DATE-TIME:20240116T085000Z
DTEND;VALUE=DATE-TIME:20240116T091000Z
DTSTAMP;VALUE=DATE-TIME:20260916T084415Z
UID:indico-contribution-11-281@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Liudmyla Sidletskaya (Odesa State Environmental Univ
 ersity)\nOne of the primary tasks of ensuring the safety of objects in con
 tact with polluting objects (for example\, radiation waste) is to assess t
 he risks associated with the possible spread of impurities over long dista
 nces. Experiments that were carried out on a real natural scale\, in which
  the migration of an impurity injected into a layer including a network of
  migration channels was studied under natural conditions\, showed that in 
 such heterogeneous media\, the tracer concentration profiles are significa
 ntly asymmetric. In particular\, they have an asymmetry strongly shifted t
 owards the flow\, in which the decrease in the impurity concentration does
  not correspond to the classical Fickian law of molecular diffusion and oc
 curs not according to an exponential law\, but rather according to a power
  law [1\,2]. Such an anomalous nature of the dispersion of impurities (for
  example\, radionuclides or other polluting components\, such as heavy met
 al atoms) during natural filtration in highly heterogeneous layers is dang
 erous due to the possibility of their migration over longer distances than
  follows from estimates made based on of the classical diffusion model.\nM
 odels with fractional spatial derivatives used in theoretical works to des
 cribe such experiments are\, as a rule\, limited to the one-dimensional ca
 se and are not directly applicable to the calculation of natural processes
  in three-dimensional anisotropic media. To solve this problem\, a concept
  for using multidimensional stochastic random walk models can be proposed\
 , including modeling Lévy flights in the space of alpha-stable random pro
 cesses [3].\nAlpha-stable random processes are processes characterized by 
 infinitely divisible scenarios (trajectories)\, which are\, in a certain s
 ense\, an attractor for all other processes.\nIf\, for example\, we consid
 er the well-known Kolmogorov equation [4] as a control equation in the one
 -dimensional case for different values of the control parameter\, then for
  some certain values of it\, it reduces to the usual diffusion equation. A
 t the same time\, there is such an interval of numerical values of the con
 trol parameter in which it turns into the diffusion equation with fraction
 al derivatives (fractional diffusion equation). And\, if the process chara
 cterized by the Gaussian distribution describes a random walk of a particl
 e that does not make long (super-diffusive) movements\, then under certain
  conditions we obtain distributions that describe so-called “Lévy fligh
 ts”\, which are suitable for modeling the movement of impurities through
  a system of channels in a given medium (matrix).\nIn the context describe
 d above\, for the problems of parameterization of experimental measurement
  data\, this work directly proposes a phenomenological expression for the 
 impurity concentration function\, which depends on a small number of param
 eters and allows the description of the migration process in both classica
 l diffusion and large-scale (super-diffusion) modes.\n\n1. Xiaoying Zhang\
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  Phys Rev Lett\, 2008. 101:058101.\n\nhttps://indico.bitp.kiev.ua/event/11
 /contributions/281/
LOCATION:BITP & Zoom
URL:https://indico.bitp.kiev.ua/event/11/contributions/281/
END:VEVENT
END:VCALENDAR
