TY - JOUR
T1 - Effects of geometrical spin frustration on triangular spin tubes formed in CsCrF4 and α-KCrF4
AU - Manaka, Hirotaka
AU - Etoh, Toshiya
AU - Honda, Yuta
AU - Iwashita, Naoki
AU - Ogata, Kenichi
AU - Terada, Norio
AU - Hisamatsu, Toru
AU - Ito, Masakazu
AU - Narumi, Yasuo
AU - Kondo, Akihiro
AU - Kindo, Koichi
AU - Miura, Yoko
PY - 2011/8
Y1 - 2011/8
N2 - 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 α-KCrF 4, 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 1.5K, 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 α-KCrF4, successive magnetic phase transitions occurred at TN1 = 2.5(1) K and at TN2 = 4.0(1) K because superexchange interactions through three Cr-F-Cr paths in each non-equilateral triangle lost their equilibrium.
AB - 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 α-KCrF 4, 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 1.5K, 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 α-KCrF4, successive magnetic phase transitions occurred at TN1 = 2.5(1) K and at TN2 = 4.0(1) K because superexchange interactions through three Cr-F-Cr paths in each non-equilateral triangle lost their equilibrium.
KW - CsCrF
KW - Electron spin resonance
KW - Frustrated magnets
KW - Heat capacity
KW - High-field magnetization
KW - Magnetic susceptibility
KW - Triangular spin tubes
KW - X-ray diffraction
KW - α-KCrF
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U2 - 10.1143/JPSJ.80.084714
DO - 10.1143/JPSJ.80.084714
M3 - Article
AN - SCOPUS:80051585705
SN - 0031-9015
VL - 80
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 8
M1 - 084714
ER -