TY - JOUR
T1 - First-order metal–semiconductor transition triggered by rattling transition in tetrahedrite Cu12Sb4S13
T2 - Cu-nuclear magnetic resonance studies
AU - Matsui, Takashi
AU - Matsuno, Haruki
AU - Kotegawa, Hisashi
AU - Tou, Hideki
AU - Suekuni, Koichiro
AU - Hasegawa, Takumi
AU - Tanaka, Hiromi I.
AU - Takabatake, Toshiro
N1 - Funding Information:
Acknowledgements T.M. and H.T. gratefully acknowledge Dr. H. Funashima for his valuable comments. This work was supported by JSPS KAKENHI Grant Numbers 15H05885 (J-Physics), 15H05882 (J-Physics), 18H04321 (J-Physics), 26400359, 15H05745, and 15H03689. This work was also partly supported by CREST JST Grant No. JPMJCR16Q6.
Publisher Copyright:
©2019 The Physical Society of Japan
PY - 2019
Y1 - 2019
N2 - Tetrahedrite Cu12Sb4S13 shows a metal–semiconductor transition (MST) at TMST = 85 K. We have studied the mechanism of the MST by measurements of Cu-NMR. Above TMST, the Cu-NMR spectrum consists of signals from a tetrahedral Cu(1) 12d site and a trigonally coordinated Cu(2) 12e site. Analyses of the spectra at 95 and 20 K yield NMR and nuclear quadrupole resonance (NQR) parameters above and below TMST. The Cu(1) signal does not show clear quadrupole splitting, which remains unchanged on cooling across TMST. On the other hand, the Cu(2) signal at T > TMST clearly shows the quadrupole splitting characterized by a quadrupole frequency νQ(2) ≈ 18.6 MHz and an asymmetry parameter η(2) ≈ 0.03. Below TMST, the values of νQ(2) and η(2) change markedly. Such marked changes in NQR parameters provide evidence of a remarkable change in the local electronic structure around the Cu(2) site. Together with νQ from NMR spectra and that from first-principles calculation, we conclude that the Cu(2) atoms are displaced from the sulfur triangles below TMST. We also found that the NMR Knight shift and the spin–lattice relaxation rate divided by temperature, 1=T1T, for the Cu(1) signal markedly change below TMST, which is ascribable to the reduction in the electronic density of states at the Fermi level.
AB - Tetrahedrite Cu12Sb4S13 shows a metal–semiconductor transition (MST) at TMST = 85 K. We have studied the mechanism of the MST by measurements of Cu-NMR. Above TMST, the Cu-NMR spectrum consists of signals from a tetrahedral Cu(1) 12d site and a trigonally coordinated Cu(2) 12e site. Analyses of the spectra at 95 and 20 K yield NMR and nuclear quadrupole resonance (NQR) parameters above and below TMST. The Cu(1) signal does not show clear quadrupole splitting, which remains unchanged on cooling across TMST. On the other hand, the Cu(2) signal at T > TMST clearly shows the quadrupole splitting characterized by a quadrupole frequency νQ(2) ≈ 18.6 MHz and an asymmetry parameter η(2) ≈ 0.03. Below TMST, the values of νQ(2) and η(2) change markedly. Such marked changes in NQR parameters provide evidence of a remarkable change in the local electronic structure around the Cu(2) site. Together with νQ from NMR spectra and that from first-principles calculation, we conclude that the Cu(2) atoms are displaced from the sulfur triangles below TMST. We also found that the NMR Knight shift and the spin–lattice relaxation rate divided by temperature, 1=T1T, for the Cu(1) signal markedly change below TMST, which is ascribable to the reduction in the electronic density of states at the Fermi level.
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U2 - 10.7566/JPSJ.88.054710
DO - 10.7566/JPSJ.88.054710
M3 - Article
AN - SCOPUS:85067235940
SN - 0031-9015
VL - 88
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 5
M1 - 054710
ER -