{"title":"Current-induced circular dichroism on metallic surfaces: A first-principles study.","authors":"Farzad Mahfouzi, Mark D Stiles, Paul M Haney","doi":"10.1103/physrevb.111.014415","DOIUrl":null,"url":null,"abstract":"<p><p>We use <i>ab initio</i> calculations to evaluate the current-induced optical response and orbital moment accumulation at the surfaces of metallic films. These two quantities are related by a sum rule that equates the circular dichroic absorption integrated over frequency to the gauge-invariant self-rotation contribution to the orbital magnetization, <math> <msub> <mrow> <mover><mrow><mi>M</mi></mrow> <mo>→</mo></mover> </mrow> <mrow><mtext>SR</mtext></mrow> </msub> </math> . In typical ferromagnets, <math> <msub> <mrow> <mover><mrow><mi>M</mi></mrow> <mo>→</mo></mover> </mrow> <mrow><mtext>SR</mtext></mrow> </msub> </math> is a good approximation to the total orbital magnetization. We compute the current-induced <math> <msub> <mrow> <mover><mrow><mi>M</mi></mrow> <mo>→</mo></mover> </mrow> <mrow><mtext>SR</mtext></mrow> </msub> </math> for a Pt thin film and compare it to the current-induced orbital moment accumulation calculated with the atom-centered approximation (ACA). We find significant differences: the size of <math> <msub> <mrow> <mover><mrow><mi>M</mi></mrow> <mo>→</mo></mover> </mrow> <mrow><mtext>SR</mtext></mrow> </msub> </math> is, in general, larger than the ACA orbital moment accumulation by an order of magnitude and includes substantial finite-size effects. The differences between the two quantities caution against interpreting optical measurements with models utilizing the ACA. Finally, we compute the total surface <math> <msub> <mrow> <mover><mrow><mi>M</mi></mrow> <mo>→</mo></mover> </mrow> <mrow><mtext>SR</mtext></mrow> </msub> </math> and ACA orbital moment accumulation as a function of layer thickness. For both quantities, the length scale at which the total surface accumulation saturates is on the order of the mean free path and longer than the length scale of their spatial profiles.</p>","PeriodicalId":48701,"journal":{"name":"Physical Review B","volume":"111 1","pages":""},"PeriodicalIF":3.2000,"publicationDate":"2025-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11833748/pdf/","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review B","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevb.111.014415","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
We use ab initio calculations to evaluate the current-induced optical response and orbital moment accumulation at the surfaces of metallic films. These two quantities are related by a sum rule that equates the circular dichroic absorption integrated over frequency to the gauge-invariant self-rotation contribution to the orbital magnetization, . In typical ferromagnets, is a good approximation to the total orbital magnetization. We compute the current-induced for a Pt thin film and compare it to the current-induced orbital moment accumulation calculated with the atom-centered approximation (ACA). We find significant differences: the size of is, in general, larger than the ACA orbital moment accumulation by an order of magnitude and includes substantial finite-size effects. The differences between the two quantities caution against interpreting optical measurements with models utilizing the ACA. Finally, we compute the total surface and ACA orbital moment accumulation as a function of layer thickness. For both quantities, the length scale at which the total surface accumulation saturates is on the order of the mean free path and longer than the length scale of their spatial profiles.
期刊介绍:
Physical Review B (PRB) is the world’s largest dedicated physics journal, publishing approximately 100 new, high-quality papers each week. The most highly cited journal in condensed matter physics, PRB provides outstanding depth and breadth of coverage, combined with unrivaled context and background for ongoing research by scientists worldwide.
PRB covers the full range of condensed matter, materials physics, and related subfields, including:
-Structure and phase transitions
-Ferroelectrics and multiferroics
-Disordered systems and alloys
-Magnetism
-Superconductivity
-Electronic structure, photonics, and metamaterials
-Semiconductors and mesoscopic systems
-Surfaces, nanoscience, and two-dimensional materials
-Topological states of matter