Weijie Zhao (1427515)R. M. Ribeiro (1886395)Minglin Toh (1823854)Alexandra Carvalho (1501945)Christian Kloc (1473742)A. H. Castro Neto (1501951)Goki Eda (1400284)
It has been well-established that\nsingle layer MX<sub>2</sub> (M\n= Mo, W and X = S, Se) are direct gap semiconductors with band edges\ncoinciding at the K point in contrast to their indirect gap multilayer\ncounterparts. In few-layer MX<sub>2</sub>, there are two valleys along\nthe Γ–K line with similar energy. There is little understanding\non which of the two valleys forms the conduction band minimum (CBM)\nin this thickness regime. We investigate the conduction band valley\nstructure in few-layer MX<sub>2</sub> by examining the temperature-dependent\nshift of indirect exciton photoluminescence peak. Highly anisotropic\nthermal expansion of the lattice and the corresponding evolution of\nthe band structure result in a distinct peak shift for indirect transitions\ninvolving the K and Λ (midpoint along Γ-K) valleys. We\nidentify the origin of the indirect emission and concurrently determine\nthe relative energy of these valleys.
Arnulf Jäger‐WaldauMartha Ch. Lux‐SteinerErnst Bucher
Chiara Massera (547887)Gernot Frenking (1569796)
Werner E. van ZylJosé M. López‐de‐LuzuriagaJohn P. FacklerRichard J. Staples
Jeongho Yeon (1406326)Sang-Hwan Kim (527119)Sau Doan Nguyen (1985821)Hana Lee (445860)P. Shiv Halasyamani (1261704)
Junghwan Do (2102317)Ranko P. Bontchev (2425492)Allan J. Jacobson (1644922)