BEGIN:VCALENDAR
VERSION:2.0
PRODID:-//CERN//INDICO//EN
BEGIN:VEVENT
SUMMARY:Long-range hops in a two-species reaction-diffusion system: renorm
 alization group and numerical simulations
DTSTART;VALUE=DATE-TIME:20211221T095000Z
DTEND;VALUE=DATE-TIME:20211221T101000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-226@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Dmytro Shapoval (Institute of Condensed Matter Physi
 cs\, National Academy of Sciences of Ukraine\, 1 Svientsitskii Street\, UA
  -- 79011 Lviv\, Ukraine \\\\ ${\\mathbb L}^4$ Collaboration \\& Doctoral 
 College for the Statistical Physics of Complex Systems\, Leipzig-Lorraine-
 Lviv-Coventry)\nWe consider the reaction-diffusion system of two-species w
 ith an anomalous superdiffusion undergoing the annihilation and coagulatio
 n reactions $A + A \\to (0\, A)$ as well as the trapping reaction $A + B \
 \to A$. The superdiffusion is modeled via long-ranged Lévy flights repres
 ented by random walks with step-lengths obeying a Lévy distribution $P(r)
  = r^{- d - \\sigma}$ (a heavy-tailed probability distribution) with contr
 ol parameter $0\n\nhttps://indico.bitp.kiev.ua/event/8/contributions/226/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/226/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Pseudopotential method for description of positron annihilation in
  spherically symmetric potential
DTSTART;VALUE=DATE-TIME:20211221T101000Z
DTEND;VALUE=DATE-TIME:20211221T103000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-236@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Marina Vorona (Institute of Applied Physics NAS of U
 kraine\, Sumy\, Ukraine)\nThe radiation resistance is the key issue for th
 e creation of new structural elements for new-generation nuclear reactors 
 and the operation extension of existing nuclear power plants. The study of
  the mechanisms of formation and dynamics of radiation defects is of consi
 derable scientific interest. The initial stage of the evolution of radiati
 on defects is the production of point-type defects. One of the most effect
 ive methods for studying point defects is spectroscopy of positron lifetim
 e\, which depends on the electron distribution. Despite the rather simple 
 idea\, its practical implementation is associated with both certain techni
 cal difficulties\, and the development of a general process theory. The me
 thod of positron annihilation spectroscopy (PAS) includes measurement of p
 ositron lifetime\, determination of probabilities of 3γ and 2γ positron 
 annihilation\, influence on the main characteristics of annihilation of va
 rious external factors [1-3]. The PAS method is used to study the electron
  structure of the material and the concentrations of point and extended de
 fects. Local formations (defects) are characterized by reduction of electr
 on density compared to defect-free regions\, so the lifetime of the positr
 on is longer in this defect. Each defect is corresponded its own lifetime 
 and the intensity of the corresponding component in the total experimental
  spectrum\, which determined by the concentration of such defects [1-3]. T
 he positron annihilation rate is determined by the overlap of the electron
  and positron densities in the region of the positron localization. It als
 o depends on the cross section of the electron-positron pair annihilation 
 process.\nA series of methods have been developed to study the electronic 
 structure of matter. They all have their advantages and disadvantages and 
 differ in the required initial data. For this problem\, we considered the 
 pseudopotential method \, which allows us to build the potential of the po
 sitron-vacancy interaction. The method idea suppose the replacement of the
  atom potential by a weak potential with the same amplitude of conduction 
 electrons scattering. The method is based on the factorization of the posi
 tron wave function into an energy-independent basic function and the smoot
 h envelope (pseudo-wave) function. Thus\, the annihilation process of the 
 positron in a spherically symmetric potential can be described.\n\n[1]. We
 st\, R. N. Positron Studies of Lattice Defectsin Metals. Positrons in Soli
 ds\, 1979\, p. 89-144.\n[2]. Puska M.J.\, Nieminen R.M .. Theory of positr
 onsin solids and on solid surfaces // Reviews of Modern Physics. 1994\, v.
  66\, p. 841-897.\n[3]. Grafutin I.\, Prokopyev E.P. Application of positr
 on annihilation spectroscopy to study the structure of matter\, Physics-Us
 pekhi (2002)\,45(1):59.\n\nhttps://indico.bitp.kiev.ua/event/8/contributio
 ns/236/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/236/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Merging of spinning binary black holes in globular clusters
DTSTART;VALUE=DATE-TIME:20211222T084500Z
DTEND;VALUE=DATE-TIME:20211222T090500Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-219@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Margarita Sobolenko (Main Astronomical Observatory N
 AS of Ukraine)\nCurrently over 50 gravitational events from compact binari
 es were reported by LIGO-Virgo consortium. We see Gravitational Waves (GW)
  as a new and very powerful informational channel. The current GW observat
 ions contain the Binary Black Hole (BH) systems key orbital parameters\, s
 uch as mass\, semi-major axis\, eccentricity and even the possible spins o
 f the BH's. The next 3G generation of ground-based observatories (Einstein
  Telescope\, Cosmic Explorer) will have the opportunity to work with GWs d
 uring multiple cycles. It can significantly improve the estimations of ind
 ividual components parameters of BH's. Based on our current high resolutio
 n direct N-body modelling of the Milky Way typical Star Cluster systems dy
 namical evolution we try to numerically estimate the influence of individu
 al spins values\, orientations and orbital eccentricities on GW waveforms 
 and observed time-frequency maps during multiple cycles for BH binary merg
 ers. In our\, up to date\, N-body dynamical simulations we use the high or
 der relativistic post-Newtonian corrections for the BH binary particles (3
 .5 post-Newtonian (PN) terms including spin-spin and spin-orbit terms). In
  the current work we present the GW waveforms catalogue which covers the l
 arge parameter space in mass ratios 0.05 - 0.82 and extreme possible indiv
 idual spin cases.\n\nhttps://indico.bitp.kiev.ua/event/8/contributions/219
 /
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/219/
END:VEVENT
BEGIN:VEVENT
SUMMARY:First results of iHKM at RHIC BES energies: measuring shear viscos
 ity of QGP
DTSTART;VALUE=DATE-TIME:20211222T133000Z
DTEND;VALUE=DATE-TIME:20211222T135000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-221@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Musfer Adzhymambetov (Bogolyubov Institute for Theor
 etical Physics)\nIntegrated hydro-kinetic model was modified and first tim
 e applied to baryon-rich matter created in heavy-ion collisions at relativ
 ely low energies of RHIC BES program. The model employs a transport approa
 ch at the early and late non-equilibrium stages of evolution of the system
  and viscous hydrodynamics with smooth continuous thermalization in the mi
 ddle stage of near-equilibrium expansion of quark-gluon plasma.  First res
 ults for $p_T$ spectra\, elliptic flow\, and femtoscopy are presented. Sim
 ulations indicate that the most successful description of the existing dat
 a corresponds to the lowest possible share viscosity to entropy density ra
 tio $\\eta/s=1/4\\pi$ and fast thermalization with $\\tau_{th}\\sim 0.5$fm
 /$c$.\n\nhttps://indico.bitp.kiev.ua/event/8/contributions/221/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/221/
END:VEVENT
BEGIN:VEVENT
SUMMARY:The estimation of pion and kaon maximal emission times in $5.02A$ 
 TeV collisions at the LHC
DTSTART;VALUE=DATE-TIME:20211222T131000Z
DTEND;VALUE=DATE-TIME:20211222T133000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-238@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Volodymyr Shapoval (Bogolyubov Institute for Theoret
 ical Physics)\nIn [1] a simple method allowing one to estimate the times o
 f maximal emission for pions and kaons\,created in the LHC Pb+Pb collision
 s at $\\sqrt{s_{NN}}=2.76$~TeV\, based on the combined fitting of their $p
 _T$ spectra and the dependences of longitudinal femtoscopy radii on the pa
 ir transverse mass\, $R_{\\mathrm{long}}(m_T)$\, was proposed and tested w
 ithin the hydrokinetic model (HKM)\, able to simulate the process of the m
 atter evolution in course of a relativistic heavy-ion collision. The entir
 e evolution process is described as passing in several stages within the m
 odel (the initial state formation\, the hydrodynamical expansion of contin
 uous medium\, the matter particlization\, and the final "afterburner" hadr
 on cascade stage). The proposed method was successfully applied to the ana
 lysis of the experimental data by the ALICE Collaboration~[2].\nIn the cur
 rent work the same method is applied to the femtoscopy analysis of Pb+Pb c
 ollisions at a higher LHC energy\, $\\sqrt{s_{NN}}=5.02$~TeV\, within an i
 mproved model version - the integrated hydrokinetic model (iHKM)\, which\,
  in particular\, additionally includes the simulation of the pre-thermal s
 tage of the system's evolution and viscous (instead of previously used ide
 al) hydrodynamics for the description of (quasi)equilibrated expansion of 
 nearly thermalized quark-gluon matter. \nThe obtained fitting results for 
 pion and kaon maximal emission times in the three centrality classes are c
 onsistent with the corresponding approximate time values\, estimated based
  on the model emission function graphs~[3]. Thus\, the method can be propo
 sed for use in the experimental analysis of A+A collisions at the current 
 LHC energy. The extracted maximal emission time values decrease\, when one
  goes from central to non-central events. The kaons are emitted later than
  pions\, mainly due to the $K^*(892)$ resonance decay contribution to the 
 total kaon yield. The $m_T$ scaling between pions and kaons gets broken be
 cause of the strong transverse collective flow at the hydrodynamical stage
  and the intensive hadron-hadron scatterings at the post-hydrodynamical st
 age of the collision.\n\n[1] Yu.M. Sinyukov\, V.M. Shapoval\, V.Yu. Naboka
 \, Nucl. Phys. A $\\textbf{946}$\, 227 (2016).\n[2] J. Adam $\\textit{et a
 l.}$ (ALICE Collaboration)\, Phys. Rev. C $\\textbf{96}$\, 064613 (2017).\
 n[3] V.M. Shapoval\, Yu.M. Sinyukov\, Nucl. Phys. A $\\textbf{1016}$\, 122
 322 (2021).\n\nhttps://indico.bitp.kiev.ua/event/8/contributions/238/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/238/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Critical point and Bose-Einstein condensation in pion matter
DTSTART;VALUE=DATE-TIME:20211222T125000Z
DTEND;VALUE=DATE-TIME:20211222T131000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-231@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Vladimir Kuznietsov (Taras Shevchenko National Unive
 rsity of Kyiv)\nThe Bose-Einstein condensation and the liquid-gas first-or
 der phase transition are studied in the interacting pion matter. Two pheno
 menological models are used: the mean-field model and the hybrid model. Fr
 ee model parameters are fixed by fitting the lattice QCD data on the pion 
 Bose condensate density at zero temperature. In spite of some minor differ
 ences\, the two models demonstrate an identical qualitative and very close
  quantitative behavior for the thermodynamic functions and electric charge
  fluctuations. A peculiar property of the considered models is an intersec
 tion of the Bose-Einstein condensation line and the line of the first-orde
 r phase transition at the critical endpoint.\n\nhttps://indico.bitp.kiev.u
 a/event/8/contributions/231/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/231/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Constraining baryon annihilation in the hadronic phase of heavy-io
 n collisions via event-by-event fluctuations
DTSTART;VALUE=DATE-TIME:20211222T123000Z
DTEND;VALUE=DATE-TIME:20211222T125000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-230@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleh Savchuk (Bogolyubov Institute for Theoretical P
 hysics of the National Academy of Sciences of Ukraine)\nWe point out that 
 the variance of net-baryon distribution normalized by the Skellam distribu
 tion baseline\, $\\kappa_2[B-\\bar{B}]/B+\\bar{B}$\, is sensitive to the p
 ossible modification of (anti)baryon yields due to $B\\bar{B}$ annihilatio
 n in the hadronic phase. The corresponding measurements can thus place str
 ingent limits on the magnitude of the $B\\bar{B}$ annihilation and its inv
 erse reaction. We perform Monte Carlo simulations of the hadronic phase in
  Pb-Pb collisions at the LHC via the recently developed subensemble sample
 r + UrQMD afterburner and show that the effect survives in net-proton fluc
 tuations\, which are directly accessible experimentally. The available exp
 erimental data of the ALICE Collaboration on net-proton fluctuations disfa
 vors a notable suppression of (anti)baryon yields in $B\\bar{B}$ annihilat
 ions predicted by the present version of UrQMD if only global baryon conse
 rvation is incorporated. On the other hand\, the annihilations improve the
  data description when local baryon conservation is imposed. The two effec
 ts can be disentangled by measuring $\\kappa_2[B+\\bar{B}]/B+\\bar{B}$\, w
 hich at the LHC is notably suppressed by annihilations but virtually unaff
 ected by baryon number conservation.\n\nhttps://indico.bitp.kiev.ua/event/
 8/contributions/230/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/230/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Phase diagram of interacting pion matter and isospin charge fluctu
 ations
DTSTART;VALUE=DATE-TIME:20211222T121000Z
DTEND;VALUE=DATE-TIME:20211222T123000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-223@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Roman Poberezhnyuk (Bogolyubov Institute for Theoret
 ical Physics of the National Academy of Sciences of Ukraine)\nEquation of 
 state and electric (isospin) charge fluctuations are studied for matter co
 mposed of interacting pions. The pion matter is described by self interact
 ing scalar fields via a $\\phi^4-\\phi^6$ type Lagrangian.  The mean-field
  approximation is used and interaction parameters are fixed by fitting lat
 tice QCD results on the isospin density as a function of the isospin chemi
 cal potential at zero temperature. Two scenarios for fixing the model para
 meters - with and without the first order phase transition are considered\
 , both yielding a satisfactory description of the lattice data. Thermodyna
 mic functions and isospin charge fluctuations are studied and systematical
 ly compared for these two scenarios\, yielding qualitative differences in 
 the behavior of isospin charge susceptibilities. These differences can be 
 probed by lattice simulations at temperatures $T \n\nhttps://indico.bitp.k
 iev.ua/event/8/contributions/223/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/223/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Influence of cluster polarization on spectrum and elastic processe
 s in $^6$LI
DTSTART;VALUE=DATE-TIME:20211222T115000Z
DTEND;VALUE=DATE-TIME:20211222T121000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-234@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Nursultan Kalzhigitov (Al-Farabi Kazakh National Uni
 versity)\nThe aim of the present report is to study nature of resonance st
 ate in $^6$Li within an extended three-cluster model. It is well-known tha
 t the nucleus $^6$Li has two sets of resonance states. The first set is fo
 rmed by low-energy resonance states which lie close to the α+d decay thre
 shold and are of positive parity. There are two very narrow and three broa
 d resonance states in the first set. The second set of resonance states co
 nsists of high-energy resonance states of negative parity. They are very b
 road and reside above the $^3$H+$^3$He decay threshold. Different microsco
 pic and semi-microscopic models have been used to study resonance states i
 n $^6$Li. As a rule\, they have been applied to investigate either low-ene
 rgy or only high-energy resonance states. In the present report we study b
 oth sets of resonance states within one microscopic model. This model was 
 formulated in Ref. [1] and is a three-cluster version of the resonating gr
 oup method. To study resonance states of $^6$Li within a large energy rang
 e the model was advanced to take into account two three-cluster configurat
 ions α+p+n and t+d+p. This allows us to involve in calculations all domin
 ant binary channels\, namely\, α+d\, $^5$He+p\, $^5$Li+n and $^3$H+$^3$He
 . Besides\, these three-cluster configurations also allow us to describe m
 ore correctly (adequately) the internal structure of d\, $^5$He\, $^5$Li\,
  $^3$He which are represented as a two-cluster configuration p+n\, $^4$He+
 n\, $^4$He+p\, d+p\, respectively. \nCalculations of discrete and continuo
 us spectrum states of $^6$Li are performed with a nucleon-nucleon potentia
 l which was suggested by Tang and coworkers and is known as the Minnesota 
 potential [2]. Parameters of the model and the nucleon-nucleon potential w
 ere selected to reproduce the ground state energy of $^6$Li. The present m
 odel with these parameters fairly good reproduces the energies and widths 
 of the observed resonance states. The dominant decay channels are found fo
 r all resonance states. The hierarchy of channels depending on their impac
 t on the energy of the ground and resonance states is established. It is s
 hown that the cluster polarization\, associated with the ability of cluste
 rs d\, $^5$He\, $^5$Li\, $^3$He to change their size and shape\, plays an 
 important role in formation of the ground state and low- and high-energy r
 esonances in $^6$Li.\n\n[1] V. S. Vasilevsky\, F. Arickx\, J. Broeckhove\,
  and T. P. Kovalenko\, «A microscopic three-cluster model with nuclear po
 larization applied to the resonances of $^7$Be and the reaction $^6$Li(p\,
 $^3$He)$^4$He»\, Nucl. Phys. A\, vol. 824\, pp. 37-57\, 2009.\n\n[2] D. R
 . Thompson\, M. LeMere\, and Y. C. Tang\, «Systematic investigation of sc
 attering problems with the resonating-group method»\, Nucl. Phys.\, vol. 
 A286\, pp. 53-66\, 1977.\n\nhttps://indico.bitp.kiev.ua/event/8/contributi
 ons/234/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/234/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Relativistic density functional approach to a unified description 
 of quark-hadron matter
DTSTART;VALUE=DATE-TIME:20211222T113000Z
DTEND;VALUE=DATE-TIME:20211222T115000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-222@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleksii Ivanytskyi (Bogolyubov Institute for Theoret
 ical Physics)\nThe principal element of a unified description of strongly 
 interacting matter within effective theories is the hadronization of quark
 s at low temperatures and baryonic densities\, while the partonic degrees 
 of freedom are being suppressed in this regime. I present a novel approach
  to attack this problem\, which is formulated based on a relativistic dens
 ity-functional motivated by the string-flip model.  Dynamical restoration 
 of chiral symmetry within this approach is ensured by construction of the 
 density functional. The low density/temperature suppression of quark degre
 es of freedom is provided by increase of the corresponding self-energy alr
 eady at the mean-field level. I also discuss the connection of the present
  approach to a Nambu-Jona-Lasinio-type model with density dependent (pseud
 o-)scalar coupling. Supplemented with the vector repulsion and diquark pai
 ring channels it is applied to model cold quark matter. The corresponding 
 couplings are limited  by confronting the results of modeling compact star
 s with quark cores to the observational data. This allows to construct the
  mean-field phase diagram of strongly interacting matter.  Effects of hadr
 onization of strongly interacting matter are considered as a result of qua
 rk correlations beyond the mean field. The correlations caused by (pseudo-
 )scalar interaction channels are considered  within the Gaussian approxima
 tion. This explicitly introduces mesonic states into the model. Their cont
 ribution to the thermodynamic potential is analyzed within the Beth–Uhle
 nbeck framework. Due to the different response of the mass spectrum of bou
 nd and continuum states to changes of the medium properties the Mott disso
 ciation of mesonic bound states occurs and is interpreted as physical mech
 anism of the deconfinement transition.\n\nhttps://indico.bitp.kiev.ua/even
 t/8/contributions/222/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/222/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Calculation of the values of the zonal component of the electric f
 ield and the velocity of transfer of the ionospheric plasma due to the ele
 ctromagnetic drift during strong magnetic storms on October 12\, 2021 and 
 November 4\, 2021
DTSTART;VALUE=DATE-TIME:20211222T100500Z
DTEND;VALUE=DATE-TIME:20211222T102500Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-237@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Vyacheslav Kolodyazhnyi (Institute of ionosphere\, N
 AS and MES of Ukraine\, Kharkiv\, Ukraine)\nIt is well known that\, under 
 quiet geomagnetic conditions\, the contribution of magnetospheric sources 
 to electric fields and currents at middle and low latitudes is small. Unde
 r undisturbed conditions\, the magnitude of the zonal component of the ele
 ctric field is several units of $mV/m$. Plasma transport in the ionosphere
  caused by these fields plays an insignificant role in contrast to plasma 
 transport due to ambipolar diffusion and neutral (thermospheric) winds. Ho
 wever\, during magnetic storms\, the penetration of electric fields to the
  heights of the ionosphere of middle latitudes takes place and\, as a cons
 equence\, an increase in the plasma velocity is observed due to the electr
 omagnetic drift $v_{EB}$. In turn\, an increase in $v_{EB}$ leads to varia
 tions in the neutral wind velocity and\, as a consequence\, to a change in
  the parameters of the global thermospheric circulation. Such a change in 
 the dynamic mode of the ionospheric plasma significantly affects the altit
 ude distribution of the ionospheric parameters.\nThe aim of this work is t
 o estimate the magnitude of the zonal component of the electric field in t
 he ionosphere over Central Europe during strong magnetic storms on October
  12 and November 4\, 2021\, as well as to calculate the velocity of plasma
  transfer in crossed electric and magnetic fields.\nThe behavior of the io
 nospheric parameters was analyzed and the values of the zonal component of
  the electric field $E_y$ and the velocity of plasma transport due to the 
 electromagnetic drift $v_{EB}$ were estimated during two strong magnetic s
 torms on October 12\, 2021 ($Kp_{max} = 6\, D_{st} = –64 ~nT$) and Novem
 ber 4\, 2021 ($Kp_{max} = 7\, D_{st} = –115 ~nT$).\nDuring the magnetic 
 storm on October 12\, 2021\, the maximum value of $|E_y|$ was equal to $27
  ~mV/m$\, and the drift velocity $v_{EB} ≈ –240~ m/s$. The magnetic st
 orm was accompanied by a strong negative ionospheric storm. According to t
 he ionosonde st. Pruhonice\, Czech Republic (50º N\, 14.6º E) during the
  main phase of the storm\, a significant decrease in $NmF2$ density by abo
 ut 60% was recorded\, and the height of $hmF2$ increased by about 40 km co
 mpared to the reference day.\nThe maximum value $|E_y|$ during the magneti
 c storm on November 4\, 2021\, it was $29~mV/m$\, and the plasma transfer 
 velocity $v_{EB}$ reached almost –$260 ~m/s$. The magnetic storm on Nove
 mber 4\, 2021 was also accompanied by a negative ionospheric storm\, durin
 g which there was a decrease in the electron density at the maximum of the
  F2 layer of the ionosphere and a significant rise in the height $hmF2$ 
 – by about 90 km.\nThe results of a comparative analysis of the experime
 ntal data of the st. Pruhonice ionosonde with calculations using the inter
 national global model of the ionosphere IRI-2016 and the regional model of
  the ionosphere CERIM IION\, developed at the Institute of Ionosphere\, ar
 e presented. It is shown that the IRI-2016 model\, even with the “F-peak
  storm model” option\, incorrectly reproduces the diurnal variations in 
 both the electron density at the maximum of the F2 layer of the ionosphere
  and for the height of this maximum $hmF2$ under disturbed conditions. The
  regional model CERIM IION\, designed for calculating the parameters of th
 e ionosphere in quiet conditions\, in comparison with the IRI-2016 model\,
  gives a more reliable forecast of variations in the main parameters of th
 e F2 layer.\nIn general\, taking into account the effects of electric fiel
 ds during magnetic storms makes it possible to refine\, analyze and physic
 ally interpret variations in the parameters of dynamic processes in the io
 nospheric plasma.\n\nhttps://indico.bitp.kiev.ua/event/8/contributions/237
 /
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/237/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Impact of asymmetric bosonic dark matter on neutron star propertie
 s
DTSTART;VALUE=DATE-TIME:20211222T094500Z
DTEND;VALUE=DATE-TIME:20211222T100500Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-218@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Edoardo Giangrandi (Centre for Physics of the Univer
 sity of Coimbra\, Coimbra\, Portugal)\nWe study an accumulation of asymmet
 ric bosonic dark matter inside neutron stars and its further impact on sta
 r's evolution. We present the conditions at which dark matter particles te
 nd to condensate in a core of the star or create an extended halo. We show
  that dark matter condensed in a core leads to a decrease of the total gra
 vitational mass and tidal deformability compared to a pure baryonic star. 
 In addition\, at some conditions self-gravitating dark matter can collapse
  gravitationally and form a black hole that can destroy the star. We study
  the range of particle mass\, coupling constant and fraction of dark matte
 r inside the neutron star that lead to the formation of a black hole insid
 e a compact star. By imposing an existing astrophysical and gravitational 
 wave constraints we set a new limit on the mass and fraction of dark matte
 r particles.\n\nhttps://indico.bitp.kiev.ua/event/8/contributions/218/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/218/
END:VEVENT
BEGIN:VEVENT
SUMMARY:The new AGN search in SDSS «MаNGA» survey
DTSTART;VALUE=DATE-TIME:20211222T092500Z
DTEND;VALUE=DATE-TIME:20211222T094500Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-220@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Kateryna Vovk (Main Astronomical Observatory\, Natio
 nal Academy of Sciences of Ukraine\,  MAO/NASU\, 27 Akademika Zabolotnoho 
 St. 03143 Kyiv\, Ukraine)\nAiming for searching outflows in AGN host' plan
 e a sample of ~600 galaxies was created from SDSS Marvin 16th Data release
 . Profiles of [OIII]5007AA spectrum line were investigated by fitting two\
 , three or four Gaussians. With significance of more then 3-sigma complica
 ted gaseous movements in some AGN hosts were revealed. The frequency of di
 fferent outflow structures were estimated.\n\nhttps://indico.bitp.kiev.ua/
 event/8/contributions/220/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/220/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Milky Way Globular Clusters:  close encounter rates with each othe
 r and with the Central Supermassive Black Hole
DTSTART;VALUE=DATE-TIME:20211222T090500Z
DTEND;VALUE=DATE-TIME:20211222T092500Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-217@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Marina Ishchenko (Main Astronomical Observatory NAS 
 of Ukraine)\nThe recent precise astrometric measurements by Gaia Data Rele
 ase 2 (DR2) provide a possibility to measure the mean proper motions for t
 he large sample of (~150) GCs of the Milky Way (MW)\, which makes it plaus
 ible to study the orbital evolution of the globular clusters (GCs) system 
 as the whole.  To explore the possible close encounters (i.e.\, possible c
 ollisions) between the GCs and Central Black Hole (CBH)\, we performed the
  orbital calculations in total of 152 GCs using our self-developed high-or
 der φ-GRAPE code. We integrated (up to 10 Gyr in look-back time) the orbi
 ts of objects with reliable positions and proper motions in five different
  external gravitational potential models. They were selected from Illustri
 s TNG-100 cosmological simulation and have a variable in time mass\, and s
 izes. Using complex criteria on impact factors\, half-mass radii and relat
 ive velocity for the collision’s detection\, we found approximately 45 p
 airs of possible GCs “collisions” for all the five external potential 
 models. We estimated 6 close encounter events with CBH on separations less
  than 100 pc from the center. The GCs sample consists of NGC 6121\, NGC 65
 44\, NGC 6642 passed close in all systems with five potential models\; Ter
 zan 9 and NGC 6981 - in systems with four potential models (not fully cros
 sing)\; Pal 2 - in systems with two potential models.\n\nhttps://indico.bi
 tp.kiev.ua/event/8/contributions/217/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/217/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Multimessenger astroparticle physics
DTSTART;VALUE=DATE-TIME:20211222T080000Z
DTEND;VALUE=DATE-TIME:20211222T084500Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-240@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Andrii Neronov (Astronomy Department\, University of
  Geneva & Université de Paris\, CNRS\, Astropaticule et Cosmologie)\nhttp
 s://indico.bitp.kiev.ua/event/8/contributions/240/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/240/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Large time and long distance asymptotics of the thermal correlator
 s of the impenetrable anyonic lattice gas
DTSTART;VALUE=DATE-TIME:20211221T132000Z
DTEND;VALUE=DATE-TIME:20211221T134000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-228@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Yurii Zhuravlov (Bogolyubov Institute for Theoretica
 l Physics of the National Academy of Sciences of Ukraine)\nWe study therma
 l correlation functions of the one-dimensional impenetrable lattice anyons
 . These correlation functions can be presented as a difference of two Fred
 holm determinants. To describe large time and long distance behavior of th
 ese objects we use effective form factor approach. The asymptotic behavior
  is different in the space-like and time-like regions. In particular\, in 
 the time-like region we observe the additional power factor on top of the 
 exponential decay. We argue that this result is universal as it is related
  to the discontinuous behavior of the phase shift function of the effectiv
 e fermions. At particular values of the anyonic parameter we recover asymp
 totics of spin-spin correlation functions in XXO quantum chain.\n\nhttps:/
 /indico.bitp.kiev.ua/event/8/contributions/228/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/228/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Calculation model of X-ray phase contrast image of tested structur
 e
DTSTART;VALUE=DATE-TIME:20211221T130000Z
DTEND;VALUE=DATE-TIME:20211221T132000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-233@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Artur Ovcharenko (Institute of Applied Physics NAS o
 f Ukraine\, Sumy\, Ukraine)\nThe X-ray phase contrast imaging (PCI) method
  allows to visualize the internal structure of objects with small density 
 gradients with high spatial resolution. The PCI technique is based on the 
 use of the phenomenon of X-ray refraction\, which leads to a change in the
  phase front of the wave that passed through the sample. As a result of su
 ch deformation of the phase front X-rays deviate from their primary direct
 ion at small angles\, the magnitude of which depends on the spatial distri
 bution of the density of matter in the object under study [1]. The phase s
 hift of X-rays can't be measured directly\, so it is converted into a inte
 nsity difference by specified ways that it can be detected. PCI technique 
 can also be combined with tomographic methods to obtain a 3D-distribution 
 of the refractive index in the sample.\nIn the presented research the calc
 ulation methods are considered for the diffraction result on the test stru
 cture. Each of sections of this structure changes the phase of the inciden
 t radiation in a specified manner. Due to the fact that Fraunhofer diffrac
 tion is observed at a considerable distance between source and screen\, it
  is one of the limit cases of the scalar Kirchhoff diffraction theory. A o
 ne-dimensional case of diffraction was considered at first\, where a linea
 r phase change occurred within each of the lattice periods. As shown by th
 e calculations for the phase lattice\, the obtained intensity distribution
  differs qualitatively from the previously considered case of the amplitud
 e lattice. Thus\, one can see the displacement of the position of the cent
 ral maximum distribution for case of a phase grating relatively the initia
 l position. Due to this\, the possibility is achieved for incident radiati
 on concentrating in the chosen position. Graphs of intensity distribution 
 for different indicator of linear phase change\, as well as for different 
 sizes of inhomogeneous section in the periodic structure of the phase latt
 ice are calculated [2]. The peculiarities of the intensity distribution of
  diffracted radiation for such test objects are shown.\n\n[1].	Paganin D. 
 Coherent x-ray optics. Oxford University Press\, 2013. 424 p.\n[2].	Kolobr
 odov V.G. Applied diffraction optics: Handbook / V.G. Kolobrodov G.S\,Tymc
 huk – К.: NTUU „KPI”\, 2014. – 312 p.\n\nhttps://indico.bitp.kiev
 .ua/event/8/contributions/233/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/233/
END:VEVENT
BEGIN:VEVENT
SUMMARY:The governing quantitative characteristics of radiation-induced se
 gregation in Fe-Cr-Ni alloy
DTSTART;VALUE=DATE-TIME:20211221T124000Z
DTEND;VALUE=DATE-TIME:20211221T130000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-232@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Roman Skorokhod (Institute of Applied Physics of Nat
 ional Academy of Sciences of Ukraine\, Sumy\, Ukraine)\nA profound consequ
 ence of irradiation (neutron\, proton\, electron and heavy ion) of metal a
 lloys is the spatial redistribution of alloy components. As a result\, the
 re are enrichment or depletion of the main\, solute and impurity component
 s of the alloy near the defect sinks. This phenomenon is called radiation-
 induced segregation (RIS) and leads to degradation of mechanical and physi
 cochemical properties of materials.\n\nThe spatial and temporal evolution 
 of the concentrations of alloy components $C_{k} $ $\\left(k=\\mathrm{Fe}\
 ,\\\, \\mathrm{Cr}\,\\\, \\mathrm{Ni}\\right)$ and point defects (PD) (vac
 ancies $C_{\\mathit{v}} $ and interstitials $C_{i} $) in the ternary conce
 ntrated Fe-Cr-Ni alloys under irradiation is described by the system of fi
 ve coupled nonlinear partial differential equations [1-3]:\n$\\begin{equat
 ion} \n\\left\\{\\begin{array}{l} {\\frac{\\partial C_{k} }{\\partial t} =
 -\\mathbf{\\nabla}\\mathbf{J}_{k} \,} \\\\ {\\frac{\\partial C_{\\mathit{v
 }} }{\\partial t} =-\\mathbf{\\nabla}\\mathbf{J}_{v} +K_{0} -R_{iv} C_{\\m
 athit{v}} C_{i} -k_{v}^{2} D_{v} \\left(C_{v} -C_{v}^{eq} \\right)\,} \\\\
  {\\frac{\\partial C_{i} }{\\partial t} =-\\mathbf{\\nabla }\\mathbf{J}_{i
 } +K_{0} -R_{iv} C_{\\mathit{v}} C_{i} -k_{i}^{2} D_{i} \\left(C_{i} -C_{i
 }^{eq} \\right).} \\end{array}\\right.  \n\\end{equation}$\n \nwhere the f
 luxes of atoms species $k$ is $\\mathbf{J}_k$\, vacancies $\\mathbf{J}_{\\
 mathit{v}} $ and interstitial $\\mathbf{J}_{i} $ defined as:\n\n$\\begin{e
 quation} \n\\mathbf{J}_{k} =-\\left(\\sum _{d=v\,i}d_{k\,d} C_{d}  \\right
 )\\mathbf{\\nabla}C_{k} +C_{k} \\left(d_{k\,v} \\mathbf{\\nabla }C_{v} -d_
 {k\,i} \\mathbf{\\nabla }C_{i} \\right)\, \n\\end{equation}$ \n$\\begin{eq
 uation} \n\\mathbf{J}_{v} =-\\sum _{k=\\mathrm{Fe}\,\\\, \\mathrm{Cr}\,\\\
 , \\mathrm{Ni}}d_{k\,v} C_{k}  \\mathbf{\\nabla }C_{v} +\\alpha C_{v} \\le
 ft(\\sum _{k=\\mathrm{Fe}\,\\\, \\mathrm{Cr}\,\\\, \\mathrm{Ni}}d_{k\,v} \
 \mathbf{\\nabla}C_{k}  \\right)\, \n\\end{equation}$ \n$\\begin{equation} 
 \n\\mathbf{J}_{i} =-\\sum _{k=\\mathrm{Fe}\,\\\, \\mathrm{Cr}\,\\\, \\math
 rm{Ni}}d_{k\,i} C_{k}  \\mathbf{\\nabla}C_{i} -\\alpha C_{i} \\left(\\sum 
 _{k=\\mathrm{Fe}\,\\\, \\mathrm{Cr}\,\\\, \\mathrm{Ni}}d_{k\,i} \\mathbf{\
 \nabla }C_{k}  \\right)\, \n\\end{equation}$ \n$K_{0} $ is the production 
 rate of radiation PD\, $R_{iv} $ is the recombination rate of PD\, $k_{v}^
 {2} $ and $k_{i}^{2} $ are the sink strengths for vacancies and interstiti
 als respectively\, $C_{v}^{eq} $ and $C_{i}^{eq} $ are the equilibrium vac
 ancy and interstitial concentrations\, $D_{v} $ and $D_{i} $ are the diffu
 sion coefficients of vacancies and interstitial\, $d_{k\,v} $ and $d_{k\,i
 } $ are the diffusivity coefficients of vacancies and interstitial. The sy
 stem with the corresponding initial and boundary conditions is solved nume
 rically (a detailed solution algorithm is given in [2]). \nThe aim of the 
 present paper is to calculate the governing quantitative characteristics o
 f RIS for Fe-20%Cr-8%Ni alloy under the irradiation. That are: concentrati
 on profiles of atoms species $k$ $C_{k} \\left(x\\right)$ and PD $C_{v\\le
 ft(i\\right)} \\left(x\\right)\\\, $\, surface concentration of atoms spec
 ies $k$ $C_{k}^{Surf} $\, the value of surface enrichment (depletion) of a
 toms species $k$ $\\Delta C_{k} $\, the full width of the concentration pr
 ofile of atoms species $k$ at half maximum enrichment (depletion) $\\mathr
 m{FWHM}_{k} $\, segregation area of atoms species $k$ $S_{k} $ and discrim
 inant of RIS of atoms species $k$ in a steady state $\\mathit{{\\mathfrak 
 D}}_{k} $. For example\, production rate dependence of surface depletion\,
  $\\mathrm{FWHM} $ and segregation area for Cr and Ni are shown in Fig. 1.
 \n\n\nFig. 1. Production rate dependence of surface Cr depletion $\\Delta 
 C_{\\mathrm{Cr}} $ and Ni enrichment $\\Delta C_{\\mathrm{Ni}} $ (solid li
 ne)\, $\\mathrm{FWHM}_{\\mathrm{Cr}} $ and $\\mathrm{FWHM}_{\\mathrm{Ni}} 
 $ (dashed line) and segregation area of Cr $S_{\\mathrm{Cr}} $ and Ni $S_{
 \\mathrm{Ni}} $ (dash-dotted line). Calculations were performed at tempera
 ture$T=400$~$\\mathrm{{}^\\circ}$C\, dose $D=10$~dpa (displacement per ato
 m).\n\nThe Authors acknowledge the support by the target research program 
 of National Academy of Sciences of Ukraine “Nuclear and radiation techno
 logies for the energy sector and social needs” for 2019-2023.\n\n[1]. Wa
 s G.S. Fundamentals of Radiation Materials Science: Metals and Alloys (2nd
  ed.). New York: Springer-Verlag\, 2017. 1002 p.\n[2]. Skorokhod R.V.\, Ko
 ropov A.V. Modeling of Radiation-Induced Segregation in Fe–Cr–Ni Alloy
 s. Physics of the Solid State. 2019. Vol. 61\, P. 2269–2276.\n[3]. Korop
 ov O.V.\, Skorokhod R.V.\, in Proceedings of Ninth International Scientifi
 c-Practical Conference “Mathematics in Modern Technical University”\, 
 Kyiv\, December\, 28–29\, 2020. Vinnytsia: Publisher FOP Kushnir Yu. V.\
 , 2021. P. 80-89. (in Ukrainian)\n\nhttps://indico.bitp.kiev.ua/event/8/co
 ntributions/232/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/232/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Entanglement measures of a frustrated spin-$1/2$ Heisenberg octahe
 dral chain within the localized-magnon approach
DTSTART;VALUE=DATE-TIME:20211221T122000Z
DTEND;VALUE=DATE-TIME:20211221T124000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-225@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Olesia Krupnitska (Institute for Condensed Matter Ph
 ysics\, NAS of Ukraine)\nWe consider the spin-1/2 antiferromagnetic Heisen
 berg model on the frustrated  octahedral chain in a presence of the extern
 al magnetic field. In a previous study [1]\, it was shown that the localiz
 ed-magnon theory [2] can be modified for simpler calculation of concurrenc
 e [3]\, which may serve as a measure of the bipartite entanglement between
  nearest-neighbor and next-nearest-neighbor spins on squares of the octahe
 dral chain. The results presented in [1] confirmed a new paradigm of the l
 ocalized-magnons concept concerned with a simple calculation of entangleme
 nt measure. This study is devoted to further application of a modified loc
 alized-magnon theory for finding other entanglement measures. To be specif
 ic\, we will consider such measures of entanglement as entanglement of for
 mation and negativity [4-5]. It could be\, thus\, concluded that the local
 ized-magnon theory can be straightforwardly adapted in order to calculate 
 the respective entanglement measures for a wide class of flat-band quantum
  Heisenberg antiferromagnets. \n\n[1] J. Strecka\, O. Krupnitska and J. Ri
 chter\, EPL\, ${\\bf 132}$ 30004 (2020).\n[2] J. Schulenburg et al.\, Phys
 . Rev. Lett. ${\\bf 88}$\, 167207 (2002).\n[3] L. Amico et al.\, Rev. Mod.
  Phys. ${\\bf 80}$\, 517 (2008).\n[4] A. Peres\, Phys. Rev. Lett. ${\\bf 7
 7}$\, 1413 (1996).\n[5] G. Vidal and R.F. Werner\, Phys. Rev. A $\\bf65$\,
  032314 (2002).\n\nhttps://indico.bitp.kiev.ua/event/8/contributions/225/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/225/
END:VEVENT
BEGIN:VEVENT
SUMMARY:The charge and the dipole moment of quantized vortex structures in
  superfluid systems
DTSTART;VALUE=DATE-TIME:20211221T120000Z
DTEND;VALUE=DATE-TIME:20211221T122000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-224@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Aleksandr Konstantinov (B.Verkin Institute for Low T
 emperature Physics and Engineering  of the National Academy of Sciences of
  Ukraine)\nThe problem of the electric fields created outside a superfluid
  liquid when quantum vortices and vortex rings appear inside the system is
  solved. It is shown that in the presence of a magnetic field a quantum vo
 rtex line acquires a linear charge density. The value of the charge densit
 y depends on the angle between the circulation vector and the magnetic fie
 ld. It was found that a charge is associated with a rectilinear vortex fil
 ament\, and a dipole moment is associated with a vortex ring. It was found
  that the key role while observing of electric fields outside the system i
 s played by the shape of the surface that bounds the superfluid system. It
  was established that the polarization associated with the velocity field 
 of the vortex ring does not cause the appearance of an electric field outs
 ide an infinite cylindrical capillary with a circular cross section in the
  case when the capillary axis coincides with the ring axis. If the system 
 does not have such a high symmetry and the axis of the ring does not coinc
 ide with the axis of the capillary\, the electric field outside the system
  is nonzero. The considered vortex structures can be generated by flows an
 d can be associated with the transition of the system to a quantum turbule
 nt state. For a laminar counterflow state of a superfluid system in a cyli
 ndrical circular capillary the electric potential outside the system is id
 entically equal to zero [1\,2]. Therefore\, the predicted magneto-electric
  properties of quantum vortex structures can serve as a basis for creating
  a sensitive quantum turbulent state detector for superfluid systems.\n\n[
 1] S. I. Shevchenko and A. M. Konstantinov\, JETP Letters\, 109\, 790 (201
 9).\n[2] S. I. Shevchenko and A. M. Konstantinov\, Low Temp. Phys. 46\, 48
  (2020).\n\nhttps://indico.bitp.kiev.ua/event/8/contributions/224/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/224/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Approaching the atomic radii from in a data-oriented way: how can 
 we benefit from a set of 'useless' structural properties?
DTSTART;VALUE=DATE-TIME:20211221T085000Z
DTEND;VALUE=DATE-TIME:20211221T091000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-229@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Tymofii Nikolaienko (Taras Shevchenko National Unive
 rsity of Kyiv)\nWe report utilization of a collection of interatomic dista
 nces\, obtained from 28 710 molecules after optimizing their geometries wi
 th quantum-chemical methods\, to introduce a new set of atomic radii for H
 \, B\, C\, N\, O\, F\, Si\, P\, S\, Cl\, Ge\, As\, Se\, Br elements. This 
 problem is tackled from a perspective which differs significantly from man
 y conventional approaches\, like van der Waals radii or the covalent ones\
 , which typically focus on introducing the atomic radii as the descriptors
  tailored for modeling specific sort of atomic contacts or bonded states f
 ound in diatomic fragments respectively. In contrast to that\, we study th
 e possibility of finding the atomic radii as parameters of a linear machin
 e-learned binary classifier\, trained to distinguish between bonded and no
 n-bonded pairs of atoms [1]. We demonstrate\, that although the distances 
 between non-bonded atomic pairs play an essential role in training this cl
 assifier\, the obtained radii still exhibit considerable similarities to t
 he conventional covalent ones [2]. We thereby provide an example for how a
  proper data-oriented treatment can turn seemingly useless data into the u
 seful one. Additional details on the procedure [3] used to create a datase
 t of interatomic distances in fully automated\, yet chemically sound manne
 r\, are discussed. \n\n\n**References**\n\n[1] T.Y. Nikolaienko and L.A. B
 ulavin\, *Comput. Theor. Chem.* (2021)\, 1204: 113389.\n[2] T.Y. Nikolaien
 ko\, V.S. Chuiko and L.A. Bulavin\, *Mol. Phys.* (2020)\, **118**: e174293
 7.\n[3] T.Y. Nikolaienko\, V.S. Chuiko and L.A. Bulavin\, *Comput. Theor. 
 Chem.* (2019)\, **1163**: 112508.\n\nhttps://indico.bitp.kiev.ua/event/8/c
 ontributions/229/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/229/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Physical mechanism of signal processing in biological neural netwo
 rks
DTSTART;VALUE=DATE-TIME:20211221T080500Z
DTEND;VALUE=DATE-TIME:20211221T085000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-239@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Alexander Vidybida (Bogolyubov Institute for Theoret
 ical Physics of the NAS of Ukraine)\nhttps://indico.bitp.kiev.ua/event/8/c
 ontributions/239/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/239/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Wave diagnostics of inhomogeneous inclusions in low-dimensional qu
 asi-periodic structures
DTSTART;VALUE=DATE-TIME:20211221T093000Z
DTEND;VALUE=DATE-TIME:20211221T095000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-235@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Liudmyla Sidletska (Odessa State Environmental Unive
 rsity)\nIn the classical work Rayleigh showed that a plane wave propagatin
 g in a one-dimensional periodic unbounded structure\, for some wavelengths
 \, undergoes total reflection at the boundaries of a fragment\, called in 
 the modern terminology accepted in the theory of such structures\, called 
 photonic crystals\, a forbidden band. In this case (by the Bloch – Floqu
 et theorem) the wave amplitude inside the periodic system decays exponenti
 ally [1].\nIn this paper\, we consider a quasi-one-dimensional\, semi-boun
 ded layered periodic structure\, in which the first (in order) layer has c
 haracteristics (refractive index\, dielectric constant) that differ from o
 ther elements. We postulate that such a construction can serve as a model\
 , for example\, of a granular chain starting from an isotopic defect (or f
 rom an impurity particle).\nIn this work\, a criterion is established for 
 the condensation of the spectrum near one of the boundaries of the forbidd
 en zone corresponding to the non-propagating wave mode. In a real prototyp
 e\, a granular chain\, such a mode (for example\, in an electromagnetic wa
 ve) is\, as it were\, "arrested" in a certain vicinity of the impurity.\nA
 s a result\, it was demonstrated how\, when the symmetry of the initial st
 ate of the system is violated\, say\, due to the formation of defects (or 
 deterministic incorporation of impurities)\, it is possible to form expone
 ntially growing and decaying modes with the formation of a separate one lo
 calized in the vicinity of the defect. The established regularities can be
  used as the basis for wave diagnostics of impurity inclusions\, as well a
 s defects in quasi-one-dimensional quasi-periodic physical systems\, for e
 xample\, inhomogeneous low-dimensional crystal structures operating on the
  principle of a wave diode [2].\n\n[1] P.G. Kevrekidis. Non-linear waves i
 n lattices: Past\, present\, future. IMA J. Appl. Math. 2011.  V. 76 (3). 
 P. 389-423\; https://doi.org/10.1093/imamat/hxr015	\n[2] S. Kasap\, H. Rud
 a\, Y. Boucher. Cambridge Illustrated Handbook of Optoelectronics and Phot
 onics. - Cambridge\, 2009 . P. 352\n\nhttps://indico.bitp.kiev.ua/event/8/
 contributions/235/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/235/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Propagation processes of correlations in the system of hard sphere
 s
DTSTART;VALUE=DATE-TIME:20211221T091000Z
DTEND;VALUE=DATE-TIME:20211221T093000Z
DTSTAMP;VALUE=DATE-TIME:20260723T004159Z
UID:indico-contribution-8-227@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Igor Gapyak (Taras Shevchenko National University of
  Kyiv)\nIn this talk we consider an approach to the description of the evo
 lution of a state by means of both reduced distribution functions and redu
 ced correlation functions\, which is based on the dynamics of correlations
  in a system of hard spheres. It should be emphasized that the generating 
 operators of solution expansions of the corresponding hierarchies of evolu
 tion equations are induced\nby the generating operators of an expansion of
  the Liouville hierarchy solution \nfor a sequence of correlation function
 s.\n$~~~~~~~$In the talk an approach to the description of the state evolu
 tion of a system of hard spheres by means of the state of a typical partic
 le determined by the generalized Enskog equation is also discussed or\, in
  other words\, the foundations of the correlations evolution description b
 y kinetic equations are considered.\n\nhttps://indico.bitp.kiev.ua/event/8
 /contributions/227/
LOCATION:Online meeting
URL:https://indico.bitp.kiev.ua/event/8/contributions/227/
END:VEVENT
END:VCALENDAR
