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Doping evolution of the charge density wave and charge density fluctuations in La2−xSrxCuO4

Charles C. Tam1,2,*, Mengze Zhu1,†,‡, Maud C. Barthélemy1, Lauren J. Cane1, Oliver J. Lipscombe1, Stefano Agrestini2, Jaewon Choi2, Mirian Garcia-Fernandez2, Ke-Jin Zhou2,§ et al.

Stephen M. Hayden1,∥

  • *Contact author: ctam@ucsb.edu
  • †Contact author: zhumen@phys.ethz.ch
  • ‡Present address: Laboratory for Solid State Physics, ETH Zürich, 8093 Zürich, Switzerland.
  • §Present address: National Synchrotron Radiation Laboratory and School of Nuclear Science and Technology, University of Science and Technology of China, Hefei 230026, China.
  • ∥Contact author: s.hayden@bristol.ac.uk

Phys. Rev. B 113, 174506 – Published 13 May, 2026

DOI: https://doi.org/10.1103/6hcs-2y4y

Abstract

Cuprate superconductors show various collective charge correlations that are intimately connected with their electronic properties. In particular, charge order in the form of an incommensurate charge density wave (CDW) order with an in-plane wave vector δCDW≈ 0.23–0.35 reciprocal lattice units appears to be universally present. In addition to CDW, dynamic charge density fluctuations (CDFs) are also present with wave vectors comparable to δCDW. CDFs are present up to ≈300K and have relatively short correlation lengths of ξ≈20Å. Here we use Cu-L3 and O-K resonant inelastic x-ray scattering (RIXS) to study the doping dependence of CDW and CDFs in La2−xSrxCuO4. We fit our data with (quasi)elastic peaks resulting from the CDW and up to four inelastic modes associated with oxygen phonons that can be strongly coupled to the CDFs. Our analysis allows us to separate the charge correlations into three components: the CDW with wave vector δ4a-CDW≈0.24 and two CDF components with δ4a-CDF≈0.24 and δ3a-CDF≈0.30. We find that for T≈Tc the CDW coexists with the CDFs for dopings near x=p≈1/8. The 4a-CDW disappears beyond x=0.16 and the 4a-CDF beyond x=0.19, leaving only a weak 3a-CDF at the highest doping studied, x=0.22. Our data suggest that low-energy charge fluctuations exist up to doping x=0.19=p★, where the pseudogap disappears; however, we find no evidence that they are associated with a quantum critical point.

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