Three-dimensional band structure of layered TiTe2:: Photoemission final-state effects

被引:40
作者
Strocov, V. N. [1 ]
Krasovskii, E. E.
Schattke, W.
Barrett, N.
Berger, H.
Schrupp, D.
Claessen, R.
机构
[1] Paul Scherrer Inst, Swiss Light Source, CH-5232 Villigen, Switzerland
[2] Univ Kiel, Inst Theoret Phys, D-24098 Kiel, Germany
[3] Donostia Int Phys Ctr, San Sebastian 20018, Basque Country, Spain
[4] CEA Saclay, DSM, DRECAM, SPCSI, F-91191 Gif Sur Yvette, France
[5] Ecole Polytech Fed Lausanne, Inst Phys Mat Complexe, CH-1015 Lausanne, Switzerland
[6] Univ Augsburg, D-86135 Augsburg, Germany
[7] Univ Wurzburg, D-97074 Wurzburg, Germany
关键词
D O I
10.1103/PhysRevB.74.195125
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Three-dimensional band structure of unoccupied and occupied states of the prototype layered material TiTe2 is determined focusing on the Gamma A line of the Brillouin zone. Dispersions and lifetimes of the unoccupied states, acting as the final states in the photoemission process, are determined from a very-low-energy electron diffraction experiment supported by first-principles calculations based on a Bloch waves treatment of multiple scattering. The experimental unoccupied states of TiTe2 feature dramatic non-free-electron effects such as multiband composition and nonparabolic dispersions. The valence band layer-perpendicular dispersions are then determined from a photoemission experiment consistently interpreted on the basis of the experimental final states to achieve control over the three-dimensional wave vector. The experimental results demonstrate the absence of the Te 4p(z)(*) Fermi surface pocket at the Gamma point and significant self-energy renormalization of the valence band dispersions. Photoemission calculations based on a Bloch waves formalism within the one-step theory reveal limitations of understanding photoemission from layered materials such as TiTe2 in terms of direct transitions.
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页数:14
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