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Electronic structure of dense solid oxygen from insulator to metal investigated with X-ray Raman scattering.


ABSTRACT: Electronic structures of dense solid oxygen have been investigated up to 140 GPa with oxygen K-edge X-ray Raman scattering spectroscopy with the help of ab initio calculations based on density functional theory with semilocal metageneralized gradient approximation and nonlocal van der Waals density functionals. The present study demonstrates that the transition energies (Pi*, Sigma*, and the continuum) increase with compression, and the slopes of the pressure dependences then change at 94 GPa. The change in the slopes indicates that the electronic structure changes at the metallic transition. The change in the Pi* and Sigma* bands implies metallic characteristics of dense solid oxygen not only in the crystal a-b plane but also parallel to the c axis. The pressure evolution of the spectra also changes at ?40 GPa. The experimental results are qualitatively reproduced in the calculations, indicating that dense solid oxygen transforms from insulator to metal via the semimetallic transition.

SUBMITTER: Fukui H 

PROVIDER: S-EPMC6815120 | biostudies-literature | 2019 Oct

REPOSITORIES: biostudies-literature

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Electronic structure of dense solid oxygen from insulator to metal investigated with X-ray Raman scattering.

Fukui Hiroshi H   Anh Le The LT   Wada Masahiro M   Hiraoka Nozomu N   Iitaka Toshiaki T   Hirao Naohisa N   Akahama Yuichi Y   Irifune Tetsuo T  

Proceedings of the National Academy of Sciences of the United States of America 20191009 43


Electronic structures of dense solid oxygen have been investigated up to 140 GPa with oxygen <i>K</i>-edge X-ray Raman scattering spectroscopy with the help of ab initio calculations based on density functional theory with semilocal metageneralized gradient approximation and nonlocal van der Waals density functionals. The present study demonstrates that the transition energies (Pi*, Sigma*, and the continuum) increase with compression, and the slopes of the pressure dependences then change at 94  ...[more]

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