Electronic structure of transition metal dichalcogenides PdTe2 and Cu0.05PdTe2 superconductors obtained by angle-resolved photoemission spectroscopy<xref ref-type="fn" rid="cpb150943fn1">*</xref>

Electronic structure of transition metal dichalcogenides PdTe₂ and Cu_0.05PdTe₂ superconductors obtained by angle-resolved photoemission spectroscopy*

Liu Yan^a), Zhao Jian-Zhou^a), Yu Li^a), Lin Cheng-Tian^b), Hu Cheng^a), Liu De-Fa^a), Peng Ying-Ying^a), Xie Zhuo-Jin^a), He Jun-Feng^a), Chen Chao-Yu^a), Feng Ya^a), Yi He-Mian^a), Liu Xu^a), Zhao Lin^a), He Shao-Long^a), Liu Guo-Dong^a), Dong Xiao-Li^a), Zhang Jun^a), Chen Chuang-Tian^c), Xu Zu-Yan^c), Weng Hong-Ming^a), Dai Xi^a), Fang Zhong^a), Zhou Xing-Jiang^a),^d)†

Calculated k _z dependence of the Fermi surface and band structures of PdTe₂ with the spin–orbit coupling and the comparison with the measurements. (a) Fermi surface of PdTe₂ measured by using the helium I ARPES. (b1)–(b4) Calculated Fermi surface at k_z = 0, 1/3, 2/3, and 1, respectively. The value of k _z is in units of π / c . (c) Band structure measured along high symmetry directions in the helium I ARPES experiment. To highlight the measured bands, we show the energy-second-derivative images of the original data. (d1)–(d4) Calculated band structures at k_z = 0, 1/3, 2/3, and 1, respectively.