Spiral spin liquid noise

H Hiroto Takahashi (The Institute for Solid State Physics, The University of Tokyo) C Chun-Chih Hsu (Department of Physics, Clarendon Laboratory, University of Oxford) F Fabian Jerzembeck (Department of Physics, Clarendon Laboratory, University of Oxford) J Jack Murphy (School of Physics, University College Cork) J Jonathan Ward (School of Physics, University College Cork) J Jack D. Enright (Department of Physics, Clarendon Laboratory, University of Oxford) J Jan Knapp (Department of Physics, Clarendon Laboratory, University of Oxford) P Pascal Puphal (Max Planck Institute for Solid State Research) M Masahiko Isobe (Max Planck Institute for Solid State Research) Y Yosuke Matsumoto (Max Planck Institute for Solid State Research) H Hidenori Takagi (Max Planck Institute for Solid State Research) J J. C. Séamus Davis (Department of Physics, Clarendon Laboratory, University of Oxford) S Stephen J. Blundell (Department of Physics, Clarendon Laboratory, University of Oxford)

Abstract

An emerging concept for identification of different types of spin liquids [C. Broholm et al. , Science 367 , eaay0668 (2020)] is through the use of spontaneous spin noise [S. Chatterjee, J. F. Rodriguez-Nieva, E. Demler, Phys. Rev. B 99 , 104425 (2019)]. Here, we develop spin noise spectroscopy for spin liquid studies by considering Ca 10 Cr 7 O 28 , a material hypothesized to be either a quantum or a spiral spin liquid (SSL). By enhancing techniques introduced for magnetic monopole noise studies [R. Dusad et al. , Nature 571 , 234–239 (2019)], we measure the time and temperature dependence of spontaneous flux Φ ( t , T ) and thus magnetization M ( t , T ) of Ca 10 Cr 7 O 28 samples. The resulting power spectral density of magnetization noise S M ω , T reveals intense spin fluctuations with S M ω , T ∝ ω - α ( T ) and 0.84 < α T < 1.04 . Both the variance σ M 2 T and the correlation function C M t , T of this spin noise undergo crossovers at a temperature T ∗ ≈ 450   mK . While predictions for quantum spin liquids are inconsistent with this phenomenology, those from Monte–Carlo simulations of a two-dimensional (2D) SSL state in Ca 10 Cr 7 O 28 yield overall quantitative correspondence with the measured frequency and temperature dependences of S M ω , T ,   C M t , T , and σ M 2 T , thus indicating that Ca 10 Cr 7 O 28 is an SSL.

Article Details

Volume / Issue Vol. 122, Issue 12
Published March 25, 2025
ISSN 0027-8424
Publisher National Academy of Sciences

Authors (13)

H

Hiroto Takahashi

The Institute for Solid State Physics, The University of Tokyo

C

Chun-Chih Hsu

Department of Physics, Clarendon Laboratory, University of Oxford

F

Fabian Jerzembeck

Department of Physics, Clarendon Laboratory, University of Oxford

J

Jack Murphy

School of Physics, University College Cork

J

Jonathan Ward

School of Physics, University College Cork

J

Jack D. Enright

Department of Physics, Clarendon Laboratory, University of Oxford

J

Jan Knapp

Department of Physics, Clarendon Laboratory, University of Oxford

P

Pascal Puphal

Max Planck Institute for Solid State Research

M

Masahiko Isobe

Max Planck Institute for Solid State Research

Y

Yosuke Matsumoto

Max Planck Institute for Solid State Research

H

Hidenori Takagi

Max Planck Institute for Solid State Research

J

J. C. Séamus Davis

Department of Physics, Clarendon Laboratory, University of Oxford

S

Stephen J. Blundell

Department of Physics, Clarendon Laboratory, University of Oxford