First-order phase transition between dimerized-antiferromagnetic and uniform-antiferromagnetic phases in Cu1xMxGeO3

T. Masuda, I. Tsukada, K. Uchinokura, Y. J. Wang, V. Kiryukhin, and R. J. Birgeneau
Phys. Rev. B 61, 4103 – Published 1 February 2000
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Abstract

We have performed detailed magnetic susceptibility measurements as well as synchrotron x-ray-diffraction studies to determine the temperature vs concentration (Tx) phase diagram of Cu1xMgxGeO3. We observe clear double peaks in the magnetic susceptibility implying two antiferromagnetic (AF) transition temperatures in samples with Mg concentrations in the range 0.0237<~x<~0.0271. We also observe a drastic change in the inverse correlation length in this concentration range by x-ray diffraction. The drastic change of the AF transition temperature as well as the disappearance of the spin-Peierls phase have been clarified; these results are consistent with a first-order phase transition between dimerized AF and uniform AF phases as reported by T. Masuda et al. [Phys. Rev. Lett. 80, 4566 (1998)]. The Tx phase diagram of Cu1xZnxGeO3 is similar to that of Cu1xMgxGeO3, which suggests that the present phase transition is universal for Cu1xMxGeO3.

  • Received 8 June 1999

DOI:https://doi.org/10.1103/PhysRevB.61.4103

©2000 American Physical Society

Authors & Affiliations

T. Masuda*,†, I. Tsukada, and K. Uchinokura

  • Department of Applied Physics, The University of Tokyo, 6th Engineering Building, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan

Y. J. Wang, V. Kiryukhin, and R. J. Birgeneau

  • Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

  • *Electronic address: tmasuda@ap.t.u-tokyo.ac.jp
  • Also at Department of Advanced Materials Science, The University of Tokyo, 6th Engineering Bldg., 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan.
  • Present address: Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan.

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Vol. 61, Iss. 6 — 1 February 2000

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