Observation of a massive phason in a charge-density-wave insulator.
Autor: | Kim S; Department of Physics, University of Illinois at Urbana-Champaign, Urbana, IL, USA.; Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Lv Y; Department of Physics, University of Illinois at Urbana-Champaign, Urbana, IL, USA.; Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Sun XQ; Department of Physics, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Zhao C; Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL, USA.; Materials Science and Engineering Department, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Bielinski N; Department of Physics, University of Illinois at Urbana-Champaign, Urbana, IL, USA.; Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Murzabekova A; Department of Physics, University of Illinois at Urbana-Champaign, Urbana, IL, USA.; Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Qu K; Department of Physics, University of Illinois at Urbana-Champaign, Urbana, IL, USA.; Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Duncan RA; Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, CA, USA.; Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, CA, USA., Nguyen QLD; Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, CA, USA.; Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, CA, USA., Trigo M; Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, CA, USA.; Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, CA, USA., Shoemaker DP; Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL, USA.; Materials Science and Engineering Department, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Bradlyn B; Department of Physics, University of Illinois at Urbana-Champaign, Urbana, IL, USA., Mahmood F; Department of Physics, University of Illinois at Urbana-Champaign, Urbana, IL, USA. fahad@illinois.edu.; Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL, USA. fahad@illinois.edu. |
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Jazyk: | angličtina |
Zdroj: | Nature materials [Nat Mater] 2023 Apr; Vol. 22 (4), pp. 429-433. Date of Electronic Publication: 2023 Mar 09. |
DOI: | 10.1038/s41563-023-01504-5 |
Abstrakt: | The lowest-lying fundamental excitation of an incommensurate charge-density-wave material is believed to be a massless phason-a collective modulation of the phase of the charge-density-wave order parameter. However, long-range Coulomb interactions should push the phason energy up to the plasma energy of the charge-density-wave condensate, resulting in a massive phason and fully gapped spectrum 1 . Using time-domain terahertz emission spectroscopy, we investigate this issue in (TaSe (© 2023. The Author(s), under exclusive licence to Springer Nature Limited.) |
Databáze: | MEDLINE |
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