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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:20260818T132306Z
UID:indico-contribution-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/
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