Related Experiment Video
Updated: Oct 15, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
Crystallographic Parity and Inverse Area Scaling in Two-Dimensional Perovskite Ferroelectric Tunnel Junctions
Aditya Nirmale1,2, Yan Li3,4, Seiichiro Izawa1,2
1Materials and Structures Laboratory, Institute of Integrated Research, Institute of Science Tokyo, Yokohama226-8503, Japan.
Abstract:
Ferroelectric tunnel junctions (FTJs) are promising for next-generation high-density non-volatile memory; however, conventional polycrystalline oxide FTJs face issues with defect-induced leakage and degraded ferroelectricity at nanometer scales. Here, we demonstrate atomically defined nanocrossbar FTJs based on single-crystalline two-dimensional (2D) Dion-Jacobson perovskite nanosheets designed to address these scaling challenges. Electrical transport measurements reveal crystallographic-parity-dependent switching behavior: odd-layered (m = 3, 5) homologs exhibit hysteretic switching consistent with ferroelectric tunnel barriers, whereas even-layered (m = 4, 6) homologs show non-switching behavior consistent with paraelectric controls. Simmons-model analysis supports direct tunneling as the dominant transport mechanism through the atomically uniform nanosheet barriers, even at the smallest junction area of 520 nm2. Notably, the tunneling electroresistance (TER) ratio increases as the junction area decreases, reaching approximately 35, consistent with the suppression of defect-induced OFF-state current inhomogeneity under nanoconfinement. These FTJs show strong non-volatile retention (extrapolated to 10 years) and reliable switching endurance (100 cycles) at room temperature. These results highlight that crystallographic layer parity and nanoconfinement-enabled defect avoidance serve as key design principles for scalable 2D ferroelectric tunnel devices and facilitate pathways toward ultra-dense post-Moore memory and neuromorphic computing architectures. This favorable scaling behavior aligns lateral miniaturization with improved memory contrast and, together with the metal-electrode nanocrossbar architecture, provides a promising basis for high-density integration if wafer-scale nanosheet assembly and reproducible interface control can be established.
More Related Videos
08:00Chemical Synthesis of Porous Barium Titanate Thin Film and Thermal Stabilization of Ferroelectric Phase by Porosity-Induced Strain
Published on: March 27, 2018
13:56Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
Published on: October 12, 2019
Related Concept Videos
Crystal Field Theory - Tetrahedral and Square Planar Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
Crystal Field Theory - Octahedral Complexes
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
Imperfections in Crystal Structure: Stoichiometric Point Defects
Crystallographic Point Groups
Symmetry Elements in a Crystal
Lattice Energies of Ionic Crystals