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Electronic structure of lithium amide
Author(s) -
N. Kamakura,
Yukiharu Takeda,
Y. Saitoh,
Hiroshi Yamagami,
Masami Tsubota,
Biswajit Paik,
Takayuki Ichikawa,
Yoshitsugu Kojima,
Takayuki Muro,
Y. Kato,
T. Kinoshita
Publication year - 2011
Publication title -
physical review b
Language(s) - English
Resource type - Journals
eISSN - 1538-4489
pISSN - 1098-0121
DOI - 10.1103/physrevb.83.033103
Subject(s) - x ray absorption spectroscopy , binding energy , electronic structure , atomic physics , band gap , absorption spectroscopy , valence (chemistry) , emission spectrum , spectral line , density of states , lithium amide , materials science , physics , molecular physics , condensed matter physics , chemistry , optics , biochemistry , quantum mechanics , astronomy , enantioselective synthesis , catalysis
The electronic structure of the insulator lithium amide (LiNH_2), which is a lightweight complex hydride being considered as a high-capacity hydrogen storage material, is investigated by N 1s soft x-ray emission spectroscopy (XES) and absorption spectroscopy (XAS). The XES and XAS spectra show a band gap between the valence and conduction bands. The valence band in the XES spectrum consists of three peaks, which extend up to -8 eV from the valence band top. The band calculation within the local-density approximation (LDA) for LiNH_2shows energetically separated three peaks in the occupied N 2p partial density of states (pDOS) and the band gap. The energy distribution of three peaks in the XES spectrum agrees with that in the calculated pDOS except for the peak at the highest binding energy, which is attributed to the strongly hybridized state between N 2p and H 1s. The XES experiment has clarified that the strongly hybridized state with H 1s in LiNH_2is located at binding energy higher than that of the LDA calculation, while the overall feature of the electronic structure of LiNH_2experimentally obtained by XES and XAS is consistent with the calculated result.

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