Effects of Geometrical Spin Frustration on Triangular Spin Tubes Formed in CsCrF4 and \alpha-KCrF4

    • Manaka Hirotaka
    • Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-0065, Japan
    • Etoh Toshiya
    • Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-0065, Japan
    • Honda Yuta
    • Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-0065, Japan
    • Iwashita Naoki
    • Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-0065, Japan

    • Ogata Kenichi
    • Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-0065, Japan
    • Terada Norio
    • Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-0065, Japan
    • Hisamatsu Toru
    • Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-0065, Japan
    • Ito Masakazu
    • Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-0065, Japan

    • Narumi Yasuo
    • Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan
    • Kondo Akihiro
    • Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan
    • Kindo Koichi
    • Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan
    • Miura Yoko
    • Suzuka National College of Technology, Suzuka, Mie 510-0294, Japan

Abstract

We conducted X-ray diffraction, magnetic susceptibility, heat capacity, high-field magnetization, and electron spin resonance experiments on high-quality polycrystalline S=3/2 compounds consisting of equilateral and non-equilateral triangular spin tubes in CsCrF4 and \alpha-KCrF4, respectively. In both compounds, geometrical spin frustration in the triangular planes coexists with one-dimensionality along the tubes. In CsCrF4, no magnetic long-range order appeared above 1.5 K, which agrees with a prior report [H. Manaka et al.: J. Phys. Soc. Jpn. 78 (2009) 093701]. In a low temperature (T) regime, T-linear component of heat capacity appeared and magnetization curves showed finite initial slopes. As a result, CsCrF4 consists of a gapless spin-liquid state encompassing resonating spin-singlet pairs not only in each equilateral triangle but also along the tubes. In contrast, for \alpha-KCrF4, successive magnetic phase transitions occurred at T_{\text{N1}} = 2.5(1) K and at T_{\text{N2}} = 4.0(1) K because superexchange interactions through three Cr--F--Cr paths in each non-equilateral triangle lost their equilibrium.

Journal

J Phys Soc Jpn  

J Phys Soc Jpn 80(8), 084714-084714-11, 2011-08-15 

The Physical Society of Japan

Codes

  • NII Article ID (NAID) :
    150000090133
  • NII NACSIS-CAT ID (NCID) :
    AA00704814
  • Text Lang :
    EN
  • ISSN :
    00319015
  • NDL Article ID :
    11201786
  • NDL Source Classification :
    ZM35(科学技術--物理学)
  • NDL Call No. :
    Z53-A404
  • Databases :
    NDL  JSAP/JPS 

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