TY - JOUR
T1 - Switching kinetics in ferroelectric zinc magnesium oxide thin films
AU - Jacques, Leonard
AU - Behrendt, Drew
AU - Ozdemir, Erdem
AU - Yousefian, Pedram
AU - Spurling, Robert Jackson
AU - Tipsawat, Pannawit
AU - Akkopru-Akgun, Betul
AU - Rappe, Andrew M.
AU - Maria, Jon Paul
AU - Yazawa, Keisuke
AU - Trolier-McKinstry, Susan
N1 - Publisher Copyright:
© 2025
PY - 2025/11/1
Y1 - 2025/11/1
N2 - The switching kinetics of RF-magnetron reactively sputtered ∼200 nm thick Zn1-xMgxO (ZMO) ferroelectric thin films with x = 0.41 and x = 0.27 prepared on Pt/Ti/SiO2/Si substrates were studied at applied fields near the coercive fields, ranging from 3.4 to 5.1 MV cm-1, and at temperatures ranging from room temperature to 100 °C. Polarization reversal in ZMO followss the Kolmogorov-Avrami-Ishibashi kinetics model for nucleation and growth at applied fields near the coercive field, and obeys an individual column switching (ICS) model at higher applied fields required to switch most of the spontaneous polarization. Switching in the high-applied field regime can be described using either the Gaussian or inverse gamma distribution functions depending on the mole fraction of magnesium in the film. The switching current transients of the high-Mg content ZMO film (x = 0.41) are always bi-modal, whereas the low Mg composition film (x = 0.27) is described by the Gaussian distribution initially following wake-up, and becomes bimodal with continued cycling. Rayleigh-like behavior of the dielectric constant revealed a simultaneous increase of the irreversible and decrease of the reversible contributions to the dielectric constant, which was ascribed to an increase in the density of mobile domain walls with cycling and resulted in faster switching.
AB - The switching kinetics of RF-magnetron reactively sputtered ∼200 nm thick Zn1-xMgxO (ZMO) ferroelectric thin films with x = 0.41 and x = 0.27 prepared on Pt/Ti/SiO2/Si substrates were studied at applied fields near the coercive fields, ranging from 3.4 to 5.1 MV cm-1, and at temperatures ranging from room temperature to 100 °C. Polarization reversal in ZMO followss the Kolmogorov-Avrami-Ishibashi kinetics model for nucleation and growth at applied fields near the coercive field, and obeys an individual column switching (ICS) model at higher applied fields required to switch most of the spontaneous polarization. Switching in the high-applied field regime can be described using either the Gaussian or inverse gamma distribution functions depending on the mole fraction of magnesium in the film. The switching current transients of the high-Mg content ZMO film (x = 0.41) are always bi-modal, whereas the low Mg composition film (x = 0.27) is described by the Gaussian distribution initially following wake-up, and becomes bimodal with continued cycling. Rayleigh-like behavior of the dielectric constant revealed a simultaneous increase of the irreversible and decrease of the reversible contributions to the dielectric constant, which was ascribed to an increase in the density of mobile domain walls with cycling and resulted in faster switching.
UR - https://www.scopus.com/pages/publications/105014611050
UR - https://www.scopus.com/pages/publications/105014611050#tab=citedBy
U2 - 10.1016/j.actamat.2025.121483
DO - 10.1016/j.actamat.2025.121483
M3 - Article
AN - SCOPUS:105014611050
SN - 1359-6454
VL - 300
JO - Acta Materialia
JF - Acta Materialia
M1 - 121483
ER -