Magnetic Properties of One-Dimensional Heisenberg Chains with Ferromagnetic-Antiferromagnetic Bond Alternation.

  • Hagiwara Masayuki
    The Institute of Physical and Chemical Research (RIKEN), Wako, Saitama 351–01 Research Center for Materials Science at Extreme Conditions, Osaka University, Toyonaka 560
  • Narumi Yasuo
    Research Center for Materials Science at Extreme Conditions, Osaka University, Toyonaka 560
  • Kindo Koichi
    Research Center for Materials Science at Extreme Conditions, Osaka University, Toyonaka 560
  • Kobayashi Tatsuo C.
    Research Center for Materials Science at Extreme Conditions, Osaka University, Toyonaka 560
  • Yamakage Hirokazu
    Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka 560
  • Amaya Kiichi
    Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka 560
  • Schumauch Georg
    The Institute of Inorganic Chemistry, University of Erlangen–Nürnberg, 91058 Erlangen, Germany

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  • Magnetic Properties of One-Dimensional

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We report the results of susceptibility and magnetization measurements on ferromagnetic-antiferromagnetic alternating chain compounds [Cu(TIM)]CuCl_4 (TIM=2, 3, 9, 10-tetramethyl-1, 3, 8, 10-tetraenecyclo-1, 4, 8, 11-tetraazatetradecane) and (4-BzpipdH)CuCl_3 (4-BzpipdH=4-benzylpiperidinium). Magnetization curves of both compounds are compared to those calculated for an S=1 linear-chain Heisenberg antiferromagnet. From the fitting of susceptibility data to a numerical formula calculated for an S=1/2 ferromagnetic-antiferromagnetic alternating chain [Inog. Chem. {33} (1994) 5171], we have estimated theantiferromagnetic exchange constant JAF/kB=2.9 K, the ferromagnetic exchange constant |JF|/kB=4.7 K and the g-value of the magnetic moment g=2.06 for the former and JAF/kB=8.8 K, |JF|/kB=38.8 K and g=2.17 for the latter, which are different from the values reportedpreviously.

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