High-pressure insulator-to-metal transition in Sr3Ir2O7 studied by x-ray absorption spectroscopy

被引:14
|
作者
Donnerer, C. [1 ,2 ]
Sala, M. Moretti [3 ]
Pascarelli, S. [3 ]
Rosa, A. D. [3 ]
Andreev, S. N. [4 ]
Mazurenko, V. V. [4 ]
Irifune, T. [5 ]
Hunter, E. C. [6 ,7 ,8 ]
Perry, R. S. [1 ,2 ]
McMorrow, D. F. [1 ,2 ]
机构
[1] UCL, London Ctr Nanotechnol, London WC1E 6BT, England
[2] UCL, Dept Phys & Astron, London WC1E 6BT, England
[3] ESRF European Synchrotron, 71 Ave Martyrs, F-38000 Grenoble, France
[4] Ural Fed Univ, Theoret Phys & Appl Math Dept, Ekaterinburg 620002, Russia
[5] Ehime Univ, Geodynam Res Ctr, 2-5 Bunkyo Cho, Matsuyama, Ehime 7908577, Japan
[6] Univ Edinburgh, SUPA, Sch Phys & Astron, Mayfield Rd, Edinburgh EH9 3JZ, Midlothian, Scotland
[7] Univ Edinburgh, Ctr Sci Extreme Condit, Mayfield Rd, Edinburgh EH9 3JZ, Midlothian, Scotland
[8] Univ Oxford, Inorgan Chem Lab, South Parks Rd, Oxford OX1 3QR, England
基金
英国工程与自然科学研究理事会;
关键词
CRYSTAL-STRUCTURE;
D O I
10.1103/PhysRevB.97.035106
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
High-pressure x-ray absorption spectroscopy was performed at the Ir L-3 and L-2 absorption edges of Sr3Ir2O7. The branching ratio of white-line intensities continuously decreases with pressure, reflecting a reduction in the angular part of the expectation value of the spin-orbit coupling operator, (L . S). Up to the high-pressure structural transition at 53 GPa, this behavior can be explained within a single-ion model, where pressure increases the strength of the cubic crystal field, which suppresses the spin-orbit induced hybridization of J(eff) = 3/2 and e(g) levels. We observe a further reduction of the branching ratio above the structural transition, which cannot be explained within a single-ion model of spin-orbit coupling and cubic crystal fields. This change in (L . S) in the high-pressure, metallic phase of Sr3Ir2O7 could arise from noncubic crystal fields or a bandwidth-driven hybridization of J(eff) = 1/2, 3/2 states and suggests that the electronic ground state significantly deviates from the J(eff) = 1/2 limit.
引用
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页数:7
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