首页|Finite Temperature Magnetism in the Triangular Lattice Antiferromagnet KErTe2
Finite Temperature Magnetism in the Triangular Lattice Antiferromagnet KErTe2
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After the discovery of the ARECh2(A=alkali or monovalent ions,RE=rare-earth,Ch=chalcogen)trian-gular lattice quantum spin liquid(QSL)family,a series of its oxide,sulfide,and selenide counterparts has been consistently reported and extensively investigated.While KErTe2 represents the initial synthesized telluride member,preserving its triangular spin lattice,it was anticipated that the substantial tellurium ions could im-part more pronounced magnetic attributes and electronic structures to this material class.This study delves into the magnetism of KErTe2 at finite temperatures through magnetization and electron spin resonance(ESR)measurements.Based on the angular momentum(J)after spin-orbit coupling(SOC)and symmetry analysis,we obtain the magnetic effective Hamiltonian to describe the magnetism of Er3+in R(3)m space group.Applying the mean-field approximation to the Hamiltonian,we can simulate the magnetization and magnetic heat capacity of KErTe2 in paramagnetic state and determine the crystalline electric field(CEF)parameters and partial exchange interactions.The relatively narrow energy gaps between the CEF ground state and excited states exert a sig-nificant influence on the magnetism.For example,small CEF excitations can result in a significant broadening of the ESR linewidth at 2 K.For the fitted exchange interactions,although the values are small,given a large angular momentum J=15/2 after SOC,they still have a noticeable effect at finite temperatures.Notably,the heat capacity data under different magnetic fields along the c axis direction also roughly match our calculated results,further validating the reliability of our analytical approach.These derived parameters serve as crucial tools for future investigations into the ground state magnetism of KErTe2.The findings presented herein lay a foundation for exploration of the intricate magnetism within the triangular-lattice delafossite family.
刘维维、张政、闫大禹、李建树、张志涛、籍建葶、金峰、石友国、张清明
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Department of Physics,Renmin University of China,Beijing 100872,China
Beijing National Laboratory for Condensed Matter Physics,and Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China
Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions,High Magnetic Field Laboratory,Chinese Academy of Sciences,Hefei 230031,China
School of Physical Science and Technology,Lanzhou University,Lanzhou 730000,China
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National Science Foundation of ChinaNational Science Foundation of ChinaNational Key Research and Development Program of ChinaStrategic Priority Research Program of the Chinese Academy of SciencesSynergetic Extreme Condition User Facility(SECUF)
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