4.8 Article

Predictive Materials Design of Magnetic Random-Access Memory Based on Nanoscale Atomic Structure and Element Distribution

Journal

NANO LETTERS
Volume 19, Issue 12, Pages 8621-8629

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.nanolett.9b03190

Keywords

Voltage-controlled magnetic anisotropy; perpendicular magnetic anisotropy; tunneling magnetoresistance; crystal structure; element distribution; magnetic tunnel junction

Funding

  1. NSF Nanosystems Engineering Research Center for Translational Applications of Nanoscale Multiferroic Systems (TANMS)
  2. Phase II NSF Small Business Innovation Research award
  3. NSF [ECCS-1554011]
  4. Energy Frontier Research Center for Spins and Heat in Nanoscale Electronic Systems (SHINES)

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Magnetic tunnel junctions (MTJs) capable of electrical read and write operations have emerged as a canonical building block for nonvolatile memory and logic. However, the cause of the widespread device properties found experimentally in various MTJ stacks, including tunneling magnetoresistance (TMR), perpendicular magnetic anisotropy (PMA), and voltage-controlled magnetic anisotropy (VCMA), remains elusive. Here, using high-resolution transmission electron microscopy and energy-dispersive Xray spectroscopy, we found that the MTJ crystallization quality, boron diffusion out of the CoFeB fixed layer, and minimal oxidation of the fixed layer correlate with the TMR. As with the CoFeB free layer, seed layer diffusion into the free layer/MgO interface is negatively correlated with the interfacial PMA, whereas the metal-oxides concentrations in the free layer correlate with the VCMA. Combined with formation enthalpy and thermal diffusion analysis that can explain the evolution of element distribution from MTJ stack designs and annealing temperatures, we further established a predictive materials design framework to guide the complex design space explorations for high-performance MTJs. On the basis of this framework, we demonstrate experimentally high PMA and VCMA values of 1.74 mJ/m(2) and 115 fJ/V.m(-1) with annealing stability above 400 degrees C.

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