2018Applied Physics LettersRequires access

The band structure of the quasi-one-dimensional layered semiconductor TiS3(001)

Hemian Yi, Takashi Komesu, Simeon Gilbert, Guanhua Hao, Andrew J. Yost, Alexey Lipatov, Alexander Sinitskii, J. Ávila, Kai Chen, M. C. Asensio, P. A. Dowben

Open publisher page 53 citations

Abstract

The experimental mapping of the band structure of TiS3(001), by momentum resolution nanospot angle resolved photoemission, is presented. The experimental band structure, derived from angle-resolved photoemission, confirms that the top of the valence band is at the center of the Brillouin zone. This trichalcogenide has a rectangular surface Brillouin zone where the effective hole mass along the chain direction is −0.95 ± 0.09 me, while perpendicular to the chain direction, the magnitude of the effective hole mass is much lower at −0.37 ± 0.1 me. The placement of the valence band well below the Fermi level suggests that this is an n-type semiconductor.

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What this paper is about

The experimental mapping of the band structure of TiS3(001), by momentum resolution nanospot angle resolved photoemission, is presented. The experimental band structure, derived from angle-resolved photoemission, confirms that the top of the valence band is at the center of the Brillouin zone. This trichalcogenide has a rectangular surface Brillouin zone where the effective hole mass along the chain direction is −0.95 ± 0.09 me, while perpendicular to the chain direction, the magnitude of the effective hole mass is much lower at −0.37 ± 0.1 me. The placement of the valence band well below the Fermi level suggests that this is an n-type semiconductor.

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Available abstract

The experimental mapping of the band structure of TiS3(001), by momentum resolution nanospot angle resolved photoemission, is presented. The experimental band structure, derived from angle-resolved photoemission, confirms that the top of the valence band is at the center of the Brillouin zone. This trichalcogenide has a rectangular surface Brillouin zone where the effective hole mass along the chain direction is −0.95 ± 0.09 me, while perpendicular to the chain direction, the magnitude of the effective hole mass is much lower at −0.37 ± 0.1 me. The placement of the valence band well below the Fermi level suggests that this is an n-type semiconductor.

Key concepts: Brillouin zone, Effective mass (spring–mass system), Electronic band structure, Semiconductor, Condensed matter physics, Quasi Fermi level, Angle-resolved photoemission spectroscopy, Perpendicular

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