4.6 Article

Excited-state band structure mapping

期刊

PHYSICAL REVIEW B
卷 105, 期 7, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.105.075417

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资金

  1. Max-Planck-Gesellschaft
  2. German Research Foundation (DFG), within the Emmy Noether Program [RE 3977/1, FOR1700, SPP2244, 443366970]
  3. European Research Council [ERC-2015-AdG-694097, ERC-2015-CoG-682843]
  4. Swiss National Science Foundation (SNSF) [CRSK-2_196756, P00P2_170597]
  5. Cluster of Excellence CUI: Advanced Imaging of Matter of the Deutsche Forschungsgemeinschaft [EXC 2056, 390715994]
  6. Swiss National Science Foundation (SNF) [CRSK-2_196756] Funding Source: Swiss National Science Foundation (SNF)

向作者/读者索取更多资源

This work extends the band structure mapping to the unoccupied states and the entire Brillouin zone by using a state-of-the-art light source to probe optically excited samples. The wideranging applicability and power of this approach are demonstrated, providing direct access to the energy-momentum dispersion of the excited-state spectral function.
Angle-resolved photoelectron spectroscopy is an extremely powerful probe of materials to access the occupied electronic structure with energy and momentum resolution. However, it remains blind to those dynamic states above the Fermi level that determine technologically relevant transport properties. In this work we extend band structure mapping into the unoccupied states and across the entire Brillouin zone by using a state-of-the-art high repetition rate, extreme ultraviolet femtosecond light source to probe optically excited samples. The wideranging applicability and power of this approach are demonstrated by measurements on the two-dimensional semiconductor WSe2, where the energy-momentum dispersion of valence and conduction bands are observed in a single experiment. This provides a direct momentum-resolved view, not only on the complete out-of-equilibrium band gap but also on its renormalization induced by electronic screening. Our work establishes a benchmark for measuring the band structure of materials, with direct access to the energy-momentum dispersion of the excited-state spectral function.

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