Hybridization Gap and Dresselhaus Spin Splitting in EuIr4In2Ge4
EuIr4In2Ge4 is a new intermetallic semiconductor that adopts a non‐centrosymmetric structure in the tetragonal ${I\bar 42m}$ space group with unit cell parameters a=6.9016(5) Å and c=8.7153(9) Å. The compound features an indirect optical band gap Eg=0.26(2) eV, and electronic‐structure calculations...
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Published in | Angewandte Chemie (International ed.) Vol. 54; no. 32; pp. 9186 - 9191 |
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Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
Published |
Weinheim
WILEY-VCH Verlag
03.08.2015
WILEY‐VCH Verlag Wiley Subscription Services, Inc |
Edition | International ed. in English |
Subjects | |
Online Access | Get full text |
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Summary: | EuIr4In2Ge4 is a new intermetallic semiconductor that adopts a non‐centrosymmetric structure in the tetragonal ${I\bar 42m}$ space group with unit cell parameters a=6.9016(5) Å and c=8.7153(9) Å. The compound features an indirect optical band gap Eg=0.26(2) eV, and electronic‐structure calculations show that the energy gap originates primarily from hybridization of the Ir 5d orbitals, with small contributions from the Ge 4p and In 5p orbitals. The strong spin–orbit coupling arising from the Ir atoms, and the lack of inversion symmetry leads to significant spin splitting, which is described by the Dresselhaus term, at both the conduction‐ and valence‐band edges. The magnetic Eu2+ ions present in the structure, which do not play a role in gap formation, order antiferromagnetically at 2.5 K.
An intermetallic semiconductor with a non‐centrosymmetric structure and the chemical formula EuIr4In2Ge4 is reported. The band gap is a direct result of strong IrIr bonding, and strong spin–orbit coupling effects lead to spin splitting at the conduction‐ and valence‐band edges, which is described by the Dresselhaus term. |
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Bibliography: | State of Illinois Department of Commerce and Economic Opportunity (DCEO) - No. 10-203031 MRSEC - No. DMR-1121262 We acknowledge the assistance of Prof. Danna Freedman and her research group, as well as support from the Northwestern University's International Institute for Nanotechnology and the State of Illinois Department of Commerce and Economic Opportunity (DCEO) Award (10-203031), which facilitated the magnetic measurements. This work made use of the EPIC facility (NUANCE Center-Northwestern University), which has received support through the MRSEC program (NSF DMR-1121262) at the Materials Research Center, the International Institute for Nanotechnology (IIN), and the State of Illinois, through the IIN. The work at Argonne National Laboratory was supported by the U.S. Department of Energy, Office of Science, Materials Sciences and Engineering. A.P.R. acknowledges support through an Undergraduate Research Grant administered by the Northwestern University Office of Undergraduate Research. ArticleID:ANIE201504315 ark:/67375/WNG-G1LXWQWL-X U.S. Department of Energy, Office of Science, Materials Sciences and Engineering istex:EF34FEF045112B4C371E645955A8D9E8AA455959 We acknowledge the assistance of Prof. Danna Freedman and her research group, as well as support from the Northwestern University’s International Institute for Nanotechnology and the State of Illinois Department of Commerce and Economic Opportunity (DCEO) Award (10‐203031), which facilitated the magnetic measurements. This work made use of the EPIC facility (NU ANCE Center‐Northwestern University), which has received support through the MRSEC program (NSF DMR‐1121262) at the Materials Research Center, the International Institute for Nanotechnology (IIN), and the State of Illinois, through the IIN. The work at Argonne National Laboratory was supported by the U.S. Department of Energy, Office of Science, Materials Sciences and Engineering. A.P.R. acknowledges support through an Undergraduate Research Grant administered by the Northwestern University Office of Undergraduate Research. ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 1433-7851 1521-3773 |
DOI: | 10.1002/anie.201504315 |