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A Janovec-Kay-Dunn-Like Behavior at Thickness Scaling in Ultra-Thin Antiferroelectric ZrO2 Films

Identifikátory výsledku

  • Kód výsledku v IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F00216208%3A11320%2F21%3A10439490" target="_blank" >RIV/00216208:11320/21:10439490 - isvavai.cz</a>

  • Výsledek na webu

    <a href="https://verso.is.cuni.cz/pub/verso.fpl?fname=obd_publikace_handle&handle=6Sd.Qhuj3s" target="_blank" >https://verso.is.cuni.cz/pub/verso.fpl?fname=obd_publikace_handle&handle=6Sd.Qhuj3s</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1002/aelm.202100485" target="_blank" >10.1002/aelm.202100485</a>

Alternativní jazyky

  • Jazyk výsledku

    angličtina

  • Název v původním jazyce

    A Janovec-Kay-Dunn-Like Behavior at Thickness Scaling in Ultra-Thin Antiferroelectric ZrO2 Films

  • Popis výsledku v původním jazyce

    Originally based on phenomenological observations, the Janovec-Kay-Dunn (JKD) scaling law has been historically used to describe the dependence of the ferroelectric coercive fields (E-c) on a critical length scale of the material, wherein the film thickness (t) is considered the length scale, and E-c proportional to t(-2/3). Here, for the first time, a JKD-type scaling behavior is reported in an antiferroelectric material, using the ultra-thin films of prototypical flourite-structure binary oxide, zirconia. In these films, a decrease in the ZrO2 layer thickness from 20 nm to 5.4 nm leads to an increase in critical fields for both nonpolar-to-polar (E-a), and polar-to-nonpolar (E-f) transitions, accompanied by a decrease in the average crystallite size, and an increase in the tetragonal distortion of the non-polar P4(2)/nmc ground state structure. Notably, the -2/3 power law as in the JKD law holds when average crystallite size (d), measured from glancing-incident X-ray diffraction, is considered as the critical length scale-i.e., E-a, E-f proportional to d(-2/3). First principles calculations suggest that the increase of tetragonality in thinner films contributes to an increase of the energy barrier for the transition from the non-polar tetragonal ground state to the field-induced polar orthorhombic phase, and in turn, an increase in E-a critical fields. These results suggest a de-stabilization of the ferroelectric phase with a decreasing thickness in antiferroelectric ZrO2, which is contrary to the observations in its fluorite-structure ferroelectric counterparts. With the recent interests in utilizing antiferroelectricity for advanced semiconductor applications, our fundamental exposition of the thickness dependence of functional responses therein can accelerate the development of miniaturized, antiferroelectric electronic memory elements for the complementary metal-oxide-semiconductor based high-volume manufacturing platforms.

  • Název v anglickém jazyce

    A Janovec-Kay-Dunn-Like Behavior at Thickness Scaling in Ultra-Thin Antiferroelectric ZrO2 Films

  • Popis výsledku anglicky

    Originally based on phenomenological observations, the Janovec-Kay-Dunn (JKD) scaling law has been historically used to describe the dependence of the ferroelectric coercive fields (E-c) on a critical length scale of the material, wherein the film thickness (t) is considered the length scale, and E-c proportional to t(-2/3). Here, for the first time, a JKD-type scaling behavior is reported in an antiferroelectric material, using the ultra-thin films of prototypical flourite-structure binary oxide, zirconia. In these films, a decrease in the ZrO2 layer thickness from 20 nm to 5.4 nm leads to an increase in critical fields for both nonpolar-to-polar (E-a), and polar-to-nonpolar (E-f) transitions, accompanied by a decrease in the average crystallite size, and an increase in the tetragonal distortion of the non-polar P4(2)/nmc ground state structure. Notably, the -2/3 power law as in the JKD law holds when average crystallite size (d), measured from glancing-incident X-ray diffraction, is considered as the critical length scale-i.e., E-a, E-f proportional to d(-2/3). First principles calculations suggest that the increase of tetragonality in thinner films contributes to an increase of the energy barrier for the transition from the non-polar tetragonal ground state to the field-induced polar orthorhombic phase, and in turn, an increase in E-a critical fields. These results suggest a de-stabilization of the ferroelectric phase with a decreasing thickness in antiferroelectric ZrO2, which is contrary to the observations in its fluorite-structure ferroelectric counterparts. With the recent interests in utilizing antiferroelectricity for advanced semiconductor applications, our fundamental exposition of the thickness dependence of functional responses therein can accelerate the development of miniaturized, antiferroelectric electronic memory elements for the complementary metal-oxide-semiconductor based high-volume manufacturing platforms.

Klasifikace

  • Druh

    J<sub>imp</sub> - Článek v periodiku v databázi Web of Science

  • CEP obor

  • OECD FORD obor

    10302 - Condensed matter physics (including formerly solid state physics, supercond.)

Návaznosti výsledku

  • Projekt

    <a href="/cs/project/EF15_003%2F0000485" target="_blank" >EF15_003/0000485: Centrum nanomateriálů pro pokročilé aplikace</a><br>

  • Návaznosti

    P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)<br>I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace

Ostatní

  • Rok uplatnění

    2021

  • Kód důvěrnosti údajů

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Údaje specifické pro druh výsledku

  • Název periodika

    Advanced Electronic Materials

  • ISSN

    2199-160X

  • e-ISSN

  • Svazek periodika

    7

  • Číslo periodika v rámci svazku

    11

  • Stát vydavatele periodika

    DE - Spolková republika Německo

  • Počet stran výsledku

    9

  • Strana od-do

    2100485

  • Kód UT WoS článku

    000694985800001

  • EID výsledku v databázi Scopus

    2-s2.0-85114672953