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)†

Band structures of Cu_0.05PdTe₂ measured along three high-symmetry directions using the helium lamp ARPES. (a) Symmetrized Fermi surface of Cu_0.05PdTe₂. The locations of the three momentum cuts are marked as blue lines #1, #2, and #3. (b)–(d) Band structures measured along three high symmetry directions: (b) K – Γ – K ′ (cut 1), (c) M – Γ – M ′ (cut 2), and (d) K ′– M ′– K (cut 3). Their corresponding energy-second-derivative images are shown in panels (e)–(g), respectively.