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The planar triangular $S=3/2$ magnet AgCrSe$_2$: magnetic frustration, short range correlations, and field tuned anisotropic cycloidal magnetic order

Authors :
Baenitz, M.
Piva, M. M.
Luther, S.
Sichelschmidt, J.
Ranjith, K. M.
Dawczak-Dȩbicki, H.
Ajeesh, M. O.
Kim, S. -J.
Siemann, G.
Bigi, C.
Manuel, P.
Khalyavin, D.
Sokolov, D. A.
Mokhtari, P.
Zhang, H.
Yasuoka, H.
King, P. D. C.
Vinai, G.
Polewczyk, V.
Torelli, P.
Wosnitza, J.
Burkhardt, U.
Schmidt, B.
Rosner, H.
Wirth, S.
Kühne, H.
Nicklas, M.
Schmidt, M.
Publication Year :
2021

Abstract

Our studies evidence an anisotropic magnetic order below $T_N = 32$~K. Susceptibility data in small fields of about 1~T reveal an antiferromagnetic (AFM) order for $H \perp c$, whereas for $H \parallel c$ the data are reminiscent of a field-induced ferromagnetic (FM) structure. At low temperatures and for $H \perp c$, the field-dependent magnetization and AC susceptibility data evidence a metamagnetic transition at $H^+ = 5$~T, which is absent for $H \parallel c$. We assign this to a transition from a planar cycloidal spin structure at low fields to a planar fan-like arrangement above $H^+$. A fully FM polarized state is obtained above the saturation field of $H_{\perp S} = 23.7$~T at 2~K with a magnetization of $M_s = 2.8$~$\mu_{\rm B}{\rm /Cr}$. For $H \parallel c$, $M(H)$ monotonously increases and saturates at the same $M_s$ value at $H_{\parallel S} = 25.1$~T at 4.2~K. Above $T_N $, the magnetic susceptibility and specific heat indicate signatures of two dimensional (2D) frustration related to the presence of planar ferromagnetic and antiferromagnetic exchange interactions. We found a pronounced nearly isotropic maximum in both properties at about $T^* = 45$~K, which is a clear fingerprint of short-range correlations and emergent spin fluctuations. Calculations based on a planar 2D Heisenberg model support our experimental findings and suggest a predominant FM exchange among nearest and AFM exchange among third-nearest neighbors. Only a minor contribution might be assigned to the antisymmetric Dzyaloshinskii-Moriya interaction possible related to the non-centrosymmetric polar space group $R3m$. Due to these competing interactions, the magnetism in AgCrSe$_{2}$, in contrast to the oxygen based delafossites, can be tuned by relatively small, experimentally accessible, magnetic fields, allowing us to establish the complete anisotropic magnetic $H-T$ phase diagram in detail.

Details

Database :
arXiv
Publication Type :
Report
Accession number :
edsarx.2109.02582
Document Type :
Working Paper
Full Text :
https://doi.org/10.1103/PhysRevB.104.134410