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Magnetic field-temperature phase diagram, exchange constants and specific heat exponents of the antiferromagnet MnNb2O6.
R, Maruthi; Ghosh, Sayandeep; Seehra, Mohindar S; Joshi, Deep C; Chowdhury, Mouli R; Medwal, Rohit; Rawat, Rajdeep S; Weise, Bruno; Thota, Subhash.
Afiliación
  • R M; Department of Physics, Indian Institute of Technology Guwahati, Assam 781039, India.
  • Ghosh S; Department of Physics, Indian Institute of Technology Guwahati, Assam 781039, India.
  • Seehra MS; Department of Physics and Astronomy, West Virginia University, Morgantown, WV 26506, United States of America.
  • Joshi DC; Department of Physics, Indian Institute of Technology Guwahati, Assam 781039, India.
  • Chowdhury MR; Department of Physics, Indian Institute of Technology Guwahati, Assam 781039, India.
  • Medwal R; National Institute of Education, Nanyang Technological University, Singapore 637616, Singapore.
  • Rawat RS; National Institute of Education, Nanyang Technological University, Singapore 637616, Singapore.
  • Weise B; Leibniz-IFW Dresden, Institute for Complex Materials, D-01069 Dresden, Germany.
  • Thota S; Department of Physics, Indian Institute of Technology Guwahati, Assam 781039, India.
J Phys Condens Matter ; 33(34)2021 Jul 01.
Article en En | MEDLINE | ID: mdl-34102622
ABSTRACT
This work presents the magnetic field-temperature (H-T) phase diagram, exchange constants, specific heat (CP) exponents and magnetic ground state of the antiferromagnetic MnNb2O6polycrystals. Temperature dependence of the magnetic susceptibilityχ(=M/H) yields the Néel temperatureTN= 4.33 K determined from the peak in the computed ∂(χT)/∂TvsTplot in agreement with the transition in theCPvsTdata atTN= 4.36 K. The experimental data ofCPvsTnearTNis fitted toCP=A|T-TN|-αyielding the critical exponentα= 0.12 (0.15) forT>TN(T 50 K toχ=χ0+C/(T-θ) withχ0= -1.85 × 10-4emu mol-1Oe-1yieldsθ= -17 K, andC= 4.385 emu K mol-1Oe-1, the latter giving magnetic momentµ= 5.920µBper Mn2+ion. This confirms the effective spinS= 5/2 andg= 2.001 for Mn2+and the dominant exchange interaction being antiferromagnetic in nature. Using the magnitudes ofθandTNand molecular field theory (MFT), the exchange constantsJ0/kB= -1.08 K for Mn2+ions along the chainc-axis andJ⊥/kB= -0.61 K as the interchain coupling perpendicular toc-axis are determined. These exchange constants are consistent with the expectedχvsTvariation for the Heisenberg linear chain. TheH-Tphase diagram, mapped using theM-Hisotherms andM-Tdata at differentHcombined with the reported data of Nielsenet al, yields a triple-pointTTP(H,T) = (18 kOe, 4.06 K). The spin-flopped state aboveTTPand the forced ferromagnetism forH> 192 kOe are used to estimate the anisotropy energyHA≈ 0.8 kOe.
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Texto completo: 1 Bases de datos: MEDLINE Idioma: En Revista: J Phys Condens Matter Asunto de la revista: BIOFISICA Año: 2021 Tipo del documento: Article País de afiliación: India

Texto completo: 1 Bases de datos: MEDLINE Idioma: En Revista: J Phys Condens Matter Asunto de la revista: BIOFISICA Año: 2021 Tipo del documento: Article País de afiliación: India