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SUMMARY:Polarization mechanism of bacteria motion in aquatic media
DTSTART;VALUE=DATE-TIME:20240926T101000Z
DTEND;VALUE=DATE-TIME:20240926T103000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-328@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleksandr Cherniak (Bogolyubov Institute for Theoret
 ical Physics)\nA new mechanism is proposed to explain the reasons for the 
 bacteria's motion in the aquatic environment. The mathematical model of th
 is mechanism is based on the hydrodynamic equations of active matter and t
 akes into account the dynamics of the environment polarization and polariz
 ation of individual bacteria. It is assumed that the flow of light and the
  active motion of dielectric regions with different refractive indices ins
 ide the bacterium lead to the formation of a nonuniform distribution of di
 pole moments at the interface between the bacterium and the aqueous medium
 . This distribution is nonequilibrium and evolves along the bacterium and 
 rotates. The interaction of this distribution with the environment due to 
 surface deformation or due to ponderomotive force leads to the bacteria's 
 motion. Such a motion can be represented as a type of turbine effect witho
 ut attachment or as an interaction of the polarization current with a chan
 ge in the local polarization of the medium. This mechanism differs signifi
 cantly from the flagella motion mechanism and can explain the motility of 
 flagellate bacteria. In addition\, such a mechanism depends on the concent
 ration of charged particles in the medium. Namely\, with an increase in th
 eir concentration\, the polarized region motion increases\, which creates 
 a greater bacterial surface deformation and causes a redistribution of pol
 arization. Moreover\, the collective bacteria motion can cause water mixin
 g.\n\nhttps://indico.bitp.kiev.ua/event/13/contributions/328/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/328/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Kinetic model of the formation of STM-induced electrofluorochromis
 m in molecular junctions
DTSTART;VALUE=DATE-TIME:20240926T095000Z
DTEND;VALUE=DATE-TIME:20240926T101000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-333@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleksiy Kapitanchuk (Bogolyubov Institute for Theore
 tical Physics\, National Academy of Sciences of Ukraine)\nExperimental dat
 a on STM-induced electroluminescence in monomolecular junctions have led t
 o the need to elucidate the physics of the formation of optoelectronic pro
 cesses at the atomic-molecular level\, taking into account both dynamic an
 d relaxation processes. A mechanism for the formation of electrofluorochro
 mism based on a kinetic model has been proposed [1]. In this model\, the d
 escription of the optoelectronic process in a photoactive molecular juncti
 on takes into account the fact that the formation of electron current and 
 electroluminescence (EL) is controlled not only by the shift of the orbita
 l energies of the molecule relative to the Fermi levels of both electrodes
 \, but also by the probability of the realization of many-body states of t
 he molecule at different values and polarities of the bias voltage. Theref
 ore\, when current and EL are generated\, the electronic states of charged
  forms of fluorophore molecules can act not only as mediators of electron 
 transfer\, but also become responsible for electrofluorochromism. It becam
 e clear that the EL in a molecular junction reflects the light emission of
  a fluorophore molecule not only between the singlet states of a neutral m
 olecule\, but also between the states of its charged forms. Thus\, we show
  that electron transfer occurs through the transmission channels associate
 d with electronic states of the neutral molecule and its cationic and anio
 nic forms\, which\, at a definite bias voltages\, are involved in electron
  transfer. The occupancies of these states are determined by kinetic proce
 sses in the molecular junction  and therefore depend on the ratio of charg
 e exchange rates between the molecule and the electrodes\, the rates of no
 n-radiative intramolecular transitions caused by inelastic interelectrode 
 tunneling of electrons\, as well as the rates of intramolecular radiative 
 transitions enhanced by the plasmonic response. Analytical results are obt
 ained using the tight-binding Hamiltonian for a molecule. The kinetic mode
 l made it possible to explain the features of EL in a monomolecular juncti
 on with the ZnPc fluorophore. Thus\, it was shown that the description of 
 EL based on the kinetic approach can serve as an effective tool for unders
 tanding the physics of optoelectronic processes in single-molecule structu
 res.\n\n1. E.Petrov\, O.Kapitanchuk\, Ye.Shevchenko\, V.Gorbach\, A.Lyubch
 ik\, Phys. Chem. Chem. Phys.\, 2024\, DOI: 10.1039/d4cp01328j\n\nhttps://i
 ndico.bitp.kiev.ua/event/13/contributions/333/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/333/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Dynamics of correlations of many colliding particles
DTSTART;VALUE=DATE-TIME:20240926T093000Z
DTEND;VALUE=DATE-TIME:20240926T095000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-297@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Viktor Gerasimenko (Institute of Mathematics NAS of 
 Ukraine)\nThe talk provides an overview of some advances in the mathematic
 al understanding of the nature of the dynamics of the correlations of many
  colliding particles. The fundamental equations of modern mathematical phy
 sics are studied\, in particular the hierarchies of the evolution equation
 s of many hard spheres and their asymptotic behavior described by kinetic 
 nonlinear equations.\n\nFirst\, an approach to describing correlations in 
 a system of colliding particles interacting as hard spheres is discussed\,
  based on a hierarchy of equations for the evolution of a sequence of corr
 elation functions that are cumulants of distribution functions\, called th
 e Lioville hierarchy. It is proven that the constructed dynamics of correl
 ations underlie the description of the dynamics of both a finite and an in
 finite number of hard spheres obeying the BBGKY hierarchies for reduced (m
 arginal) distribution functions or reduced correlation functions.\n\nThe s
 tructure of expansions representing non-perturbative solutions of the Cauc
 hy problem for these hierarchies of evolution equations is formulated. It 
 has been established that the concept of cumulants of the groups of operat
 ors of the Lioville equations underlies non-perturbative expansions of sol
 utions to the hierarchies of fundamental equations describing the evolutio
 n of observables and of the state of many hard spheres\, as well as forms 
 the basis of the kinetic description of their collective behavior.\n\nIn t
 he talk\, we also consider a new approach to the problem of a rigorous des
 cription of kinetic evolution by means of reduced (marginal) observables g
 overned by the dual BBGKY hierarchy. One of the advantages of the develope
 d approach to the derivation of kinetic equations from the underlying dyna
 mics of many particles is that it provides an opportunity to construct kin
 etic equations with initial correlations\, in particular correlations char
 acterizing the condensed states of a system\, and to describe the processe
 s of the propagation of initial correlations within suitable scaling limit
 s.\n\nReferences\n[1] Gerasimenko V I and Gapyak I V 2023 Advances in theo
 ry of evolution equations of many colliding particles. *Proc. Inst. Math. 
 NASU* **20** 729–804 doi:10.3842/trim.v20n1.528\n[2] Gerasimenko V I and
  Gapyak I V 2022 Propagation of correlations in a hard sphere system. *J S
 tat. Phys.* **189** 2 doi:10.1007/s10955-022-02958-8\n[3] Gerasimenko V I 
 and Gapyak I V 2021 Boltzmann–Grad asymptotic behavior of collisional dy
 namics. *Reviews in Math. Phys.* **33** 2130001 32 doi:10.1142/S0129055X21
 300016\n[4] Gerasimenko V I and Gapyak I V 2019 Processes of creation and 
 propagation\nof correlations in large quantum particle system. In: *Panora
 ma of Contemporary Quantum Mechanics – Concepts and Applications.* Londo
 n: InTech\, 2019 doi:10.5772/intechopen.82836\n\nhttps://indico.bitp.kiev.
 ua/event/13/contributions/297/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/297/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Development and analysis of novel integrable nonlinear dynamical s
 ystems on quasi-one-dimensional lattices. Parametrically driven nonlinear 
 system of pseudo-excitations on a two-leg ladder lattice
DTSTART;VALUE=DATE-TIME:20240926T084000Z
DTEND;VALUE=DATE-TIME:20240926T090000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-336@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleksiy O. Vakhnenko (Bogolyubov Institute for Theor
 etical Physics)\nFollowing the main principles of developing the evolution
 ary nonlinear integrable systems on quasi-one-dimensional lattices we sugg
 est the novel nonlinear integrable system of parametrically driven pseudo-
 excitations on a regular two-leg ladder lattice. The initial (prototype) f
 orm of the system is derivable in the framework of semi-discrete zero-curv
 ature equation with the spectral and evolution operators specified by the 
 properly organized 3×3 square matrices. Although the lowest conserved loc
 al densities found via the direct recursive method do not prompt us the al
 gebraic structure of system's Hamiltonian function\, but the heuristically
  substantiated search for the suitable two-stage transformation of prototy
 pe field functions to the physically motivated ones has allowed to disclos
 e the physically meaningful nonlinear integrable system with time-dependen
 t longitudinal and transverse inter-site coupling parameters. The time dep
 endencies of inter-site coupling parameters in the transformed system are 
 consistently dened in terms of the accompanying parametric driver formaliz
 ed by the set of four homogeneous ordinary linear dierential equations wit
 h the time-dependent coeficients. The physically meaningful parametrically
  driven nonlinear system permits its concise Hamiltonian formulation with 
 the two pairs of field functions serving as the two pairs of canonically c
 onjugated field amplitudes. The explicit example of oscillatory parametric
  drive is described in full mathematical details.\n\nhttps://indico.bitp.k
 iev.ua/event/13/contributions/336/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/336/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Stimulating exitable membrane of ORN with stochastic Markov proces
 s
DTSTART;VALUE=DATE-TIME:20240926T082000Z
DTEND;VALUE=DATE-TIME:20240926T084000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-358@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Oleksandr Vidybida (Bogolyubov Institute for Theoret
 ical Physics)\nExcitable membrane of olfactory receptor neuron (ORN) is po
 pulated with up to several millions of identical receptor proteins (R) abl
 e to bind / release odor (O) molecules. The affinity of R to O depends on 
 the odor presented\, and this is the initial mechanism which is recuired f
 or the olfactory selectivity to exist.\n\n\nFigure 1: Simplified R structu
 re. Modified from [3].\n\nThe affinity of R to O depends on the odor prese
 nted\, and this is the very first step the olfactory selectivity builds up
 . Recently\, [1]\, it was shown for a so called membrane-less ORN model th
 at its selectivity can be much better than that of its R. A more realistic
  ORN model should include an excitable membrane with its electric transien
 ts. This introduces time parameter into the ORN's response to stimulation.
  The latter renders inappropriate used in [1] reasoning in terms of binomi
 al distribution\, and necessitates consideration of temporal properties of
  O binding-releasing and the membrane charging-discharging-firing.\n\nIn t
 his contribution\, we develop an approach in which the number of R bound w
 ith O $n(t)$\, is modeled as a Markov stochastic process. With each bound 
 R\, \nas it is observed for insects [2]\, Fig. 1\, we associate an open ch
 annel having conductance 0.015 nS\, which injects a depolarizing current t
 hrough the membrane.\n The futher membrane evolution is governed by the le
 aky integrate-and-fire neuronal model\, see Eq. (1).\n$c_M\\frac{dV(t)}{dt
 }=-g_l(V(t)-V_{rest}) - n(t)g_{R}(V(t)-V_{e})$\,\nwhere $V(t)$ --- is the 
 membrane voltage\; $V_{rest}$ --- is the resting voltage\;\n$c_M$ --- is t
 he total capacity of ORN's membrane\;\n$g_l$ --- is the total leakage thro
 ugh it\;\n$V_{e}$ --- is the reversal potential for current through open $
 R$\;\n$n(t)$ --- is the fluctuating number of open channels at moment $t$ 
 due\nto odor molecules bound with $R$s\;\n$g_{R}$ --- is the conductance o
 f a single open channel.\n\nA fast\, very efficient method is developed fo
 r generating stochastic trajectories $n(t)$ and solving Eq. (1) numericall
 y\, see Fig. 2. The first\, introductory simulations based on this method\
 , [4]\, support the conclusion made in [1] and before\, that ORN's selecti
 vity can be much better than that of its receptors R\, provided that odors
  are presented in low concentrations.\n\n\nFigure 2: An example of realiza
 tion of stochastic process n(t) and corresponding membrane voltage\, with 
 three spikes emitted. Here\, the total number of R per the ORN is $N = 2.5
  · 10^6$\n\n[1] A. K. Vidybida\, ``Maximization of the olfactory receptor
  neuron selectivity in\n  the sub-threshold regime''\, Ukrainian Journal o
 f Physics\, vol. 68\, no.4\, p. 266\, 2023. Available: {\\tt https://doi.o
 rg/10.15407/ujpe68.4.266}\n\n[2] K. Sato\, M. Pellegrino\, T. Nakagawa\, T
 . Nakagawa\, L. B. Vosshall\, and\n  K. Touhara\, ``Insect olfactory recep
 tors are heteromeric ligand-gated ion\n  channels''\, Nature\, vol. 452\, 
 no. 7190\, pp. 1002--1006\, 2008. Available: {\\tt https://doi.org/10.1038
 /nature06850}\n\n[3] D. Wicher\, F. Miazzi\, ``Functional properties of in
 sect olfactory receptors: ionotropic receptors and odorant receptors''\, C
 ell and Tissue Research\, vol. 383(1):7-19 (2021). Available: {\\tt https:
 //doi.org/10.1007/s00441-020-03363-x}\n\n[4] A. Vidybida\, "Selectivity Ga
 in in Olfactory Receptor Neuron at Optimal Odor Concentration\," 2024 IEEE
  International Symposium on Olfaction and Electronic Nose (ISOEN)\, Grapev
 ine\, TX\, USA\, 2024\, pp. 1-3. Available: {\\tt https://ieeexplore.ieee.
 org/document/10556323}\n\nhttps://indico.bitp.kiev.ua/event/13/contributio
 ns/358/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/358/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Recursive Method for Calculating T-Matrix of Electron Scattering o
 n Arbitrary Many-Particle Clusters in Strongly Correlated Systems
DTSTART;VALUE=DATE-TIME:20240926T080000Z
DTEND;VALUE=DATE-TIME:20240926T082000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-347@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Tatiana Shatnii (G. V. Kurdyumov Institute for Metal
  Physics\, N.A.S. of Ukraine)\nThe generalized recursive method for calcul
 ating the T-matrix of electron scattering on arbitrary many-particle clust
 ers for determining the Green's function of the strongly correlated system
  is developed. This approach is extended to the studying electronic spectr
 a in both direct (Wannier) and reciprocal (Bloch) representations with tak
 ing into account the influence of atomic and magnetic correlations arising
  in the system at a temperature of 0 K. The one-band Hubbard model\, the c
 orrelated random field approximation\, and the one-site coherent potential
  approximation for the effective Hamiltonian of system are also used in th
 is approach. The spectral density in reciprocal space is calculated in the
  same way (the same scheme) as in direct space\, using the appropriate exp
 ressions for the effective Green's function\, which includes contributions
  from all crystal sublattices. Calculation of the small parameter of the c
 luster expansion of the Green's function in direct and reciprocal represen
 tations shows its smallness for different parameters of b.c.c alloys. This
  ensures the convergence of obtained recursive formulas for T-matrix of sc
 attering on many-particle clusters and the applicability of pairwise appro
 ximation for T-matrix. It should be noted that to calculate the configurat
 ion-averaged Green's function it is necessary to use at least the pairwise
  approximation of T-matrix for describing the influence of the cluster env
 ironment of each atom on the redistribution of charge and spin densities o
 n atoms\, as well as atomic and magnetic correlations. In addition\, the p
 ossibility of nanoclusters formation and their influence on the magnetic s
 tate was investigated in the b.c.c. alloy with strong electron correlation
 s. The calculation of electronic spectra in the reciprocal (as in direct) 
 representation showed the high sensitivity to the changes in the character
 istics and composition of the b.c.c. alloy including the nanoclusters form
 ation as well as to the change of resulting short-range atomic and magneti
 c orders. This method could be useful to analyze experimental data obtaine
 d\, for example\, in positron spectroscopy to study electronic structure\,
  defects\, chemical composition\, and various correlations in systems.\n**
 Key words:** Green's function for strongly correlated alloys\, recursive e
 xpression for T-matrix\, arbitrary many-particle clusters\, short-range at
 omic and magnetic ordering.\n\nhttps://indico.bitp.kiev.ua/event/13/contri
 butions/347/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/347/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Impurity-induced localized modes in parallel Josephson junction ar
 rays
DTSTART;VALUE=DATE-TIME:20240926T074000Z
DTEND;VALUE=DATE-TIME:20240926T080000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-350@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Daryna Bukatova (Bogolyubov Institute for Theoretica
 l Physics)\nWe consider inhomogeneous underdamped one-dimensional parallel
  Josephson junction arrays. Inhomogeneity is introduced either as a non-un
 iformly applied dc bias current or as variations in the junctions' critica
 l currents. We investigate the frequency of the localized modes induced by
  the presence of such inhomogeneities\, in particular the frequency's depe
 ndence on the parameters that characterise inhomogeneities.\n\nhttps://ind
 ico.bitp.kiev.ua/event/13/contributions/350/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/350/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Sagnac effect in solids
DTSTART;VALUE=DATE-TIME:20240926T072000Z
DTEND;VALUE=DATE-TIME:20240926T074000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-310@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Sergei Sharapov (Bogolyubov Institute for Theoretica
 l Physics   of the National Academy of Sciences of Ukraine  Kyiv Academic 
 University)\nThe observation of the Sagnac effect for massive material par
 ticles offers a significant enhancement in sensitivity when compared to op
 tical interferometers with equal area and angular rotation velocity. For t
 his reason\, there have been suggestions to employ solid-state interferome
 ters that rely on semiconductors and graphene. We investigate the Sagnac e
 ffect in Dirac materials governed by the relativistic-like quasiparticle d
 ispersion law and show that the fringe shift is still determined by the ma
 ss of a free electron. This confirms that graphene is indeed a promising m
 aterial for creating solid-state Sagnac interferometers. Considering monol
 ayer graphene with its linear dispersion law and comparing it with light p
 rovides a deeper understanding of the Sagnac effect.\n\nhttps://indico.bit
 p.kiev.ua/event/13/contributions/310/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/310/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Analytical Description of Size Effects\, Strains and Ferro-ionic C
 oupling in Si-Compatible Nanosized Ferroelectrics
DTSTART;VALUE=DATE-TIME:20240926T070000Z
DTEND;VALUE=DATE-TIME:20240926T072000Z
DTSTAMP;VALUE=DATE-TIME:20260723T012339Z
UID:indico-contribution-75-331@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Anna Morozovska (Institute of Physics\, National Aca
 demy of Sciences of Ukraine)\nThe analytical methods based on the Landau-G
 inzburg-Devonshire (LGD) approach and variational principle allow the anal
 ytical description of size effects\, strain and ferro-ionic coupling in lo
 w-dimensional ferroelectric materials\, such as thin films and small nanop
 articles. The validity of LGD approach is corroborated by experimental evi
 dence of the size- and strain-induced transitions as well as the related p
 henomena in the low-dimensional ferroelectric materials. For the correct d
 escription of these effects in ferroelectric thin films and small nanopart
 icles the LGD approach should be combined with the classical electrostatic
 s and elasticity theory\, and variational principle. It is important to de
 termine how the LGD expansion coefficients depend on various factors\, suc
 h as temperature\, size\, elastic stresses and/or strains\, and ionic-elec
 tronic charge density and distribution. For classical ferroelectric films 
 with a pronounced temperature-dependent and strain-dependent soft mode\, t
 he first expansion coefficients have a linear dependence on the temperatur
 e and elastic strain.\nThe significant attention is devoted to the compari
 son with experimental results and finite element modelling\, as well as on
  the theoretical predictions of the size-\, strain- and ionic- control of 
 polar and dielectric properties of nanosized ferroelectric materials.\nAs 
 the first example\, we consider ultra-thin layers and nanoflakes of van de
 r Waals ferrielectric CuInP2S6 covered by an ionic surface charge and reve
 al the appearance of polar states with relatively high polarization and st
 ored free charge\, which can mimic “mid-gap” states related with a sur
 face field-induced transfer of Cu and/or In ions in the van der Waals gap 
 [1]. The changes of the ionic screening degree and mismatch strains can in
 duce the transitions between paraelectric phase\, antiferroelectric\, ferr
 ielectric\, and ferroelectric-like states in CuInP2S6 nanoflakes. Due to t
 he emergence of manyfold-degenerated metastable states of spontaneous pola
 rization the ultra-thin layers of CuInP2S6 reveal features of the controll
 able negative capacitance effect [2]\, which make them attractive for adva
 nced electronic devices\, such as nano-capacitors and gate oxide nanomater
 ials with reduced heat dissipation.\nAs the second example\, we use the LG
 D model to quantify the strain-charge-polarization coupling in nanosized H
 fxZr1-xO2. A key factor ruling the observed polar properties of nanosized 
 HfxZr1-xO2 is the presence of the polar orthorhombic phase. This phase is 
 metastabile compared to the bulk monoclinic phase\, leading to problems wi
 th the ferroelectric phase stability in nanoscale. The electrophysical pro
 perties of the HfxZr1-xO2 thin films and nanoparticles are very sensitive 
 to the elastic strain induced by the substrate\, annealing conditions\, de
 position method\, film thickness\, content x and dopants. Depending on the
  interplay of these factors\, the nanosized HfxZr1-xO2 exhibits dielectric
 \, ferroelectric\, or antiferroelectric behavior. \nThe used model [3] inc
 orporates parametrized Landau expansion coefficients for the polar and ant
 ipolar orderings. Obtained results agrees with the recent existing experim
 ental data for HfxZr1-xO2-y thin films and oxygen-deficient HfO2-y nanopar
 ticles [4]\, namely the X-ray diffraction confirmed the formation of a fer
 roelectric orthorhombic phase in the HfO2-y nanoparticles under special fa
 vorable annealing conditions. \nThe analytical LGD approach correctly pred
 icts the phase diagrams\, ground and metastable states\, alongside the dom
 ain structure morphology\, associated polar and structural properties of H
 fxZr1-xO2-y thin films and nanoparticles with different shapes and sizes. 
 The successful application of the analytical LGD approach can be useful fo
 r the prediction of the silicon-compatible ferroelectric nanomaterials bas
 ed on HfxZr1-xO2-y. \nThe work is funded by the National Research Foundati
 on of Ukraine (projects “Manyfold-degenerated metastable states of spont
 aneous polarization in nanoferroics: theory\, experiment and perspectives 
 for digital nanoelectronics”\, grant N 2023.03/0132 and “Silicon-compa
 tible ferroelectric nanocomposites for electronics and sensors”\, grant 
 N 2023.03/0127).\n[1]. Anna N. Morozovska\, Sergei V. Kalinin\, Eugene A. 
 Eliseev\, Svitlana Kopyl\, Yulian M. Vysochanskii\, and Dean R. Evans. Fer
 ri-ionic Coupling in CuInP2S6 Nanoflakes: Polarization States and Controll
 able Negative Capacitance (2024)\, https://doi.org/10.48550/arXiv.2405.143
 68\n[2]. Anna N. Morozovska\, Eugene A. Eliseev\, Yulian M. Vysochanskii\,
  Sergei V. Kalinin\, and Maksym V. Strikha. Size Effect of Negative Capaci
 tance State and Subthreshold Swing in Van der Waals Ferrielectric Field-Ef
 fect Transistors\, https://doi.org/10.48550/arXiv.2406.13051\n[3]. Anna N.
  Morozovska\, Maksym V. Strikha\, Kyle P. Kelley\, Sergei V. Kalinin\, and
  Eugene A. Eliseev. Effective Landau-type model of a HfxZr1-xO2-graphene n
 anostructure\, Phys. Rev. Applied 20\, 054007 (2023) https://doi.org/10.11
 03/PhysRevApplied.20.054007\n[4]. Eugene A. Eliseev\, Yuri O. Zagorodniy\,
  Victor N. Pavlikov\, Oksana V. Leshchenko\, Hanna V. Shevilakova\, Mirosl
 av V. Karpec\, Andrei D. Yaremkevych\, Olena M. Fesenko\, Sergei V. Kalini
 n\, and Anna N. Morozovska. Phase diagrams and polarization reversal in na
 nosized HfxZr1-xO2-y\, AIP Advances\, 14\, 055224 (2024)\, https://doi.org
 /10.1063/5.0209123\n\nhttps://indico.bitp.kiev.ua/event/13/contributions/3
 31/
LOCATION:Bogolyubov Institute for Theoretical Physics (Section 1-4)\, Inst
 itute of Mathematics (Section 5) 322
URL:https://indico.bitp.kiev.ua/event/13/contributions/331/
END:VEVENT
END:VCALENDAR
