Chemical pressure effect on the optical conductivity of the nodal-line semimetals ZrSiY (Y = S, Se, Te) and ZrGeY (Y = S, Te)

被引:29
作者
Ebad-Allah, J. [1 ,2 ]
Afonso, J. Fernandez [3 ]
Krottenmueller, M. [1 ]
Hu, J. [4 ]
Zhu, Y. L. [5 ,6 ]
Mao, Z. Q. [5 ,6 ]
Kunes, J. [3 ,7 ]
Kuntscher, C. A. [1 ]
机构
[1] Augsburg Univ, Expt Phys 2, D-86159 Augsburg, Germany
[2] Tanta Univ, Dept Phys, Tanta 31527, Egypt
[3] TU Wien, Inst Solid State Phys, A-1020 Vienna, Austria
[4] Univ Arkansas, Dept Phys, Fayetteville, AR 72701 USA
[5] Penn State Univ, Dept Phys, University Pk, PA 16803 USA
[6] Tulane Univ, Dept Phys & Engn Phys, New Orleans, LA 70118 USA
[7] Czech Acad Sci, Inst Phys, Prague 18221, Czech Republic
基金
欧盟地平线“2020”; 欧洲研究理事会;
关键词
Optical conductivity;
D O I
10.1103/PhysRevB.99.125154
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
ZrSiS is a nodal-line semimetal, whose electronic band structure contains a diamond-shaped line of Dirac nodes. We carried out a comparative study on the optical conductivity of ZrSiS and the related compounds ZrSiSe, ZrSiTe, ZrGeS, and ZrGeTe by reflectivity measurements over a broad frequency range combined with density functional theory calculations. The optical conductivity exhibits a distinct U shape, ending at a sharp peak at around 10 000 cm(-1) for all studied compounds except for ZrSiTe. The U shape of the optical conductivity is due to transitions between the linearly dispersing bands crossing each other along the nodal line. The sharp high-energy peak is related to transitions between almost parallel bands, and its energy position depends on the interlayer bonding correlated with the c/a ratio, which can be tuned by either chemical or external pressure. For ZrSiTe, another pair of crossing bands appears in the vicinity of the Fermi level, corrugating the nodal-line electronic structure and leading to the observed difference in optical conductivity. The findings suggest that the Dirac physics in ZrXY compounds with X = Si, Ge and Y = S, Se, Te is closely connected to the interlayer bonding.
引用
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页数:8
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