4.6 Article

Band-folding-driven high tunnel magnetoresistance ratios in (111)-oriented junctions with SrTiO3 barriers

期刊

PHYSICAL REVIEW B
卷 106, 期 13, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.106.134438

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资金

  1. JSPS KAKENHI [JP22H04966, JP20H02190, JP21H01750, JP20K14782]
  2. JST CREST Integrated Devices and Systems Utilized by Information Carriers [JPMJCR21C1]
  3. Co-operative Research Project Program of the Research Institute of Electrical Communication, Tohoku University

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In this study, we theoretically investigate the tunnel magnetoresistance (TMR) effect in (111)-oriented magnetic tunnel junctions (MTJs) with SrTiO3 barriers, specifically Co/SrTiO3/Co(111) and Ni/SrTiO3/Ni(111). Our analysis combining first-principles calculations and the Landauer formula reveals that the Co-based MTJ exhibits a high TMR ratio (>500%), while the Ni-based MTJ has a smaller TMR ratio (290%). This difference is attributed to the band folding phenomenon and the half-metallic band structure in the Lambda(1) state of Co (Ni), as well as the variation in the s-orbital weights at the Fermi level.
We theoretically study the tunnel magnetoresistance (TMR) effect in (111)-oriented magnetic tunnel junctions (MTJs) with SrTiO3 barriers, Co/SrTiO3/Co(111) and Ni/SrTiO3/Ni(111). Our analysis combining the first-principles calculation and the Landauer formula shows that the Co-based MTJ has a high TMR ratio over 500%, while the Ni-based MTJ has a smaller value (290%). Since the in-plane lattice periodicity of SrTiO3 is about twice that of the primitive cell of fcc Co (Ni), the original bands of Co (Ni) are folded in the k(x)-k(y) plane corresponding to the ab plane of the MTJ supercell. We find that this band folding gives a half-metallic band structure in the Lambda(1) state of Co (Ni) and the coherent tunneling of such a half-metallic Lambda(1) state yields a high TMR ratio. We also reveal that the difference in the TMR ratio between the Co- and Ni-based MTJs can be understood by different s-orbital weights in the Lambda(1) band at the Fermi level.

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