Bulletin of the American Physical Society
APS March Meeting 2021
Volume 66, Number 1
Monday–Friday, March 15–19, 2021; Virtual; Time Zone: Central Daylight Time, USA
Session U71: Poster Session III (2:00pm - 4:00pm)
2:00 PM,
Thursday, March 18, 2021
Abstract: U71.00034 : Short-range nematic fluctuations in Sr1-xNaxFe2As2*
Presenter:
Shan Wu
(Lawrence Berkeley National Laboratory)
Authors:
Shan Wu
(Lawrence Berkeley National Laboratory)
Yu Song
(Zhejiang University)
Yu He
(Yale University)
Alex Frano
(University of California San Diego)
Ming Yi
(Rice University)
Xiang Chen
(Lawrence Berkeley National Laboratory)
Hiroshi Uchiyama
(Japan Synchrotron Radiation Research Institute)
Ahmet Alatas
(Advanced Photon Source, Argonne National Laboratory)
Ayman Said
(Advanced Photon Source, Argonne National Laboratory)
Liran Wang
(Karlsruhe Institute of Technology)
Thomas Wang
(Karlsruhe Institute of Technology)
Christoph Meingast
(Karlsruhe Institute of Technology)
Robert J Birgeneau
(Lawrence Berkeley National Laboratory)
Abundant evidence indicates that nematic fluctuations are closely related to unconventional superconductivity. For both hole- and electron-doped iron-based superconductors (FeSCs), the underdoped phase space is widely inhabited by intertwined nematic and magnetic orders. Hole-doped FeSCs, such as Sr1-xNaxFe2As2, uniquely exhibit a re-entrant tetragonal magnetic (AFM-T) phase before entering the superconducting phase in the underdoped (UD) regime. By using inelastic x-ray scattering, we observed softened transverse acoustic phonons in the UD sample that harbors the AFM-T phase, and the optimal-doped (OP) sample. By extracting both the nematic susceptibility and correlation length, we find a large nematic susceptibility persisting in the AFM-T phase, and a short nematic correlation length ξ ~ 10 Å that is much smaller than that on the electron-doped side. The OP sample manifests weaker phonon softening effect, indicative of reduced fluctuations. This result indicates that short-range nematic fluctuations may be an important ingredient favorable for superconductivity.
*Work is funded by the U.S. DOE, Office of Science, Office of Basic Energy Sciences, Materials Sciences and Engineering Division under Con- tract No. DE-AC02-05-CH11231 within the Quantum Materials Program (KC2202).
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