4.5 Article

Magnetization reversal, field-induced transitions and H-T phase diagram of Y1-xCexCrO3

期刊

出版社

IOP Publishing Ltd
DOI: 10.1088/1361-648X/ac3453

关键词

antiferromagnetism; perovskites; exchange interactions; exchange bias; Dzyaloshinskii-Moriya (DM) interaction

资金

  1. FIST programme of Department of Science and Technology, India [SR/FST/PSII-020/2009, SR/FST/PSII-037/2016]
  2. Council of Scientific and Industrial Research (CSIR), Ministry of Science and Technology, Government of India
  3. Central Instrument Facility (CIF) of the Indian Institute of Technology Guwahati
  4. Ministry of Education (MOE), Singapore [MOE2019-T2-1-058]
  5. National Research Foundation (NRF) [NRF-CRP21-2018-0003]

向作者/读者索取更多资源

In this study, a systematic investigation of the magnetic phase diagram, negative magnetization, exchange interactions, and field-induced spin-flop transitions in the distorted perovskite Y1-xCexCrO3 was conducted, revealing the unique characteristics of the Ce-incorporated system.
We report a systematic study of the magnetic phase diagram in the H-T plane, negative magnetization (NM), exchange interactions and field-induced spin-flop transitions in the distorted perovskite Y1-xCexCrO3. Locked AFM and weak-FM configurations in Gamma(4)(G(z) , F-y , A(x) ) phase of YCrO3 (S = 3/2 ground state) unlocks into the Gamma(2)(F-z , G(y) , C-x ; F-z(R),C-x(R)) phase of the canted AFM and FM structures with the dilute substitution of Ce (x >= 0.05). The asymmetric and symmetric exchange interaction (J(AS) similar to 0.11 meV and J(S) similar to 0.85 meV) between the trivalent Ce and Cr enable the positive quartic-anisotropy field (H-K4 similar to 2.85 x 10(2) Oe) along with the second order anisotropy field (H-K2 similar to 5.93 x 10(2) Oe). Unlike the pristine YCrO3 compound, the Ce incorporated system exhibits a giant fourth-order anisotropy constant (K-4 = 1.35 x 10(5) erg/c.c.) due to the asymmetric exchange interaction between the trivalent Ce-Cr which further lifts the free energy of the system and causes lag in the onset of AFM ordering showing the significant thermal hysteresis (Delta T similar to 10 K) in the field-cooled (FC)-warming measurement protocol as compared to the FC-cooling mode. The H-T phase diagram, mapped from the isothermal magnetization data and differential magnetic susceptibility data with different measurement protocols clearly distinguishes three prominent regions below the T-N (similar to 150 K), viz (i) long-range canted AFM + weak FM phase (Gamma(4) (G(z) , F-y , A(x) )), (ii) Gamma(24) mixed phase and (iii) robust Gamma(2) (F-z , G(y) , C-x ; F-z(R), C-x(R)) AFM + FM phases. Tunable spin-flopped transition (similar to 30 kOe), significant negative exchange-bias field (H-EB similar to 2.5 kOe), huge coercive field (H-C similar to 22 kOe) and large NM (Delta M similar to 280 emu/mole) are the unique characteristic features of the current investigated system.

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