Related Experiment Video
Updated: Sep 27, 2026

In Situ Transmission Electron Microscopy with Biasing and Fabrication of Asymmetric Crossbars Based on Mixed-Phased a-VOx
Published on: May 13, 2020
Thermally Enhanced Dual-Mode Resistive Switching via Interfacial Strain Engineering in SmNiO3/PMN-PT Heterostructures
1Shaanxi Key Laboratory of Intelligent Processing for Big Energy Data, School of Physics and Electronic Information, Yan'an University, Yan'an 716000, China.
Abstract:
SmNiO3 thin films on PMN-PT ferroelectric substrates enable electrically switchable strain engineering, an advantage over permanently fixed lattice-mismatch strain. However, strain-engineered resistive switching in SmNiO3 via ferroelectric substrates remains largely unexplored. Here, by stabilizing high-quality epitaxial SmNiO3 films on (011)-cut PMN-PT through a LaAlO3/SrTiO3 graded buffer interface, we demonstrate dual-mode resistive modulation in SmNiO3/PMN-PT heterostructures: reversible butterfly-shaped hysteresis under bipolar fields arising from dynamic electrostrain, and nonvolatile switching through non-180° ferroelastic domain reorientation. Moderate heating to 75 °C boosts the resistance modulation, correlated with enhanced strain output from the PMN-PT substrate near its phase transition. At the same bias of 12 kV/cm, the modulation increases from -6.4% at 25 °C to -11.9%; even at only 6 kV/cm, the modulation reaches -6.7%, exceeding the room-temperature value at 12 kV/cm. These results demonstrate the potential of SmNiO3/PMN-PT heterostructures for dual-mode resistive switching, integrating both volatile and nonvolatile modulation within a single material system through a thermally enhanced strain-coupling mechanism. This work serves as a proof-of-concept demonstration for future exploration in neuromorphic applications.
Related Concept Videos
MOSFET: Enhancement Mode
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no current...
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...

