Symmetry-breaking and spin-blockage effects on carrier dynamics in single-layer tungsten diselenide

Ro-Ya Liu, Meng-Kai Lin, Peng Chen, Takeshi Suzuki, Pip C. J. Clark, Nathan K. Lewis, Cephise Cacho, Emma Springate, Chia-Seng Chang, Kozo Okazaki, Wendy Flavell, Iwao Matsuda, and Tai-Chang Chiang
Phys. Rev. B 100, 214309 – Published 17 December 2019

Abstract

Understanding carrier creation and evolution in materials initiated by pulsed optical excitation is central to developing ultrafast optoelectronics. We demonstrate herein that the dynamic response of a system can be drastically modified when its physical dimension is reduced to the atomic scale, the ultimate limit of device miniaturization. A comparative study of single-layer (SL) tungsten diselenide (WSe2) relative to bulk WSe2 shows substantial differences in the transient response as measured by time- and angle-resolved photoemission spectroscopy (TRARPES). The conduction-band minimum in bulk WSe2, populated by optical pumping, decays promptly. The corresponding decay for SL WSe2 is much slower and exhibits two time constants. The results indicate the presence of two distinct decay channels in the SL that are correlated with the breaking of space inversion symmetry in the two-dimensional limit. This symmetry breaking lifts the spin degeneracy of the bands, which in turn causes the blockage of decay for one spin channel. The stark contrast between the single layer and the bulk illustrates the basic carrier scattering processes operating at different timescales that can be substantially modified by dimensional and symmetry-reduction effects.

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  • Received 15 February 2019
  • Revised 9 November 2019

DOI:https://doi.org/10.1103/PhysRevB.100.214309

©2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Ro-Ya Liu1,2,3,4, Meng-Kai Lin1, Peng Chen1,5,6, Takeshi Suzuki4, Pip C. J. Clark7,*, Nathan K. Lewis7, Cephise Cacho8,9, Emma Springate8, Chia-Seng Chang2, Kozo Okazaki4, Wendy Flavell7,†, Iwao Matsuda4,‡, and Tai-Chang Chiang1,§

  • 1Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801–3080, USA
  • 2Institute of Physics, Academia Sinica, Taipei, 11529, Taiwan
  • 3Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
  • 4Institute for Solid State Physics, The University of Tokyo, Chiba, 277–8581, Japan
  • 5Shanghai Center for Complex Physics, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
  • 6Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Ton University, Shanghai 200240, China
  • 7School of Physics and Astronomy and the Photon Science Institute, University of Manchester, Oxford Road, Manchester M13 9PL, United Kingdom
  • 8Central Laser Facility, STFC Rutherford Appleton Laboratory, Harwell, OX11 0QX, United Kingdom
  • 9Diamond Light Source, Harwell Campus, Didcot OX11 0DE, United Kingdom

  • *Present address: Institute for Solar Fuels Helmholtz-Zentrum Berlin für Materialien und Energie GmbH Hahn-Meitner Platz 1, D-14109 Berlin, Germany; pip.clark@helmholtz-berlin.de
  • Corresponding authors: wendy.flavell@manchester.ac.uk
  • imatsuda@issp.u-tokyo.ac.jp
  • §tcchiang@illinois.edu

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Vol. 100, Iss. 21 — 1 December 2019

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