Related Experiment Video
Updated: Sep 19, 2025

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
Published on: January 21, 2016
Mn3SnN-Based Antiferromagnetic Tunnel Junction with Giant Tunneling Magnetoresistance and Multi-States: Design and
Shiqi Liu1, Tingwei Chen1, Baochun Wu2
1State Key Laboratory of Spintronic Devices and Technologies, Hangzhou, 311305, P. R. China.
Abstract:
Antiferromagnets have attracted widespread interest due to the advantages of no stray fields and ultrafast switching dynamics, promising for next-generation high-speed, high-density memories. However, over a long period, the effective detection of antiferromagnetic (AFM) orders remained being one of the greatest challenges of its application in magnetic random access memories (MRAM) because of its zero net magnetization. Recently, the preliminary demonstration of the tunneling magnetoresistance ratio(TMR) in antiferromagnetic tunnel junctions (AFMTJ) offered a feasible solution. Here, a Mn3SnN/SrTiO3/Mn3SnN non-collinear AFMTJ is designed and its transport properties are predicted by ab initio quantum transport simulations. Due to the momentum matching between the spin-polarized Fermi surface of the Mn3SnN electrode and the low-decay-rate evanescent states of the SrTiO3 barrier, a remarkable TMR ≈1500% is generated, corresponding to a large device read margin, resulting in higher storage density. In addition, changing the relative orientation of two Mn3SnN magnetic orders leads to four non-volatile resistance states with a low resistance area (RA) of only 0.07-1.25 Ω•µm2 and three multi-state TMR of ≈500, 1000, and 1500%, suitable for high-energy-efficiency multiple-state memory application. Our work provides a promising device structure for future nonvolatile high-speed, high-density, and multiple-state AFM memories.
More Related Videos
05:39Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
09:06Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
Related Concept Videos
Ferromagnetism
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
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...
Characteristics of MOSFET
Various vital parameters influence their functionality, which is crucial for theory and electronics applications. First, channel dimensions, precisely length, and width, are pivotal. The size of these channels affects the transistor's ability to carry current and switching speeds; shorter channels typically enable...
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...
Magnetic Susceptibility and Permeability
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...