Magnetic field induced one-magnon Raman scattering in the magnon Bose-Einstein condensation phase of TlCuCl3

Haruhiko Kuroe, Kouhei Kusakabe, Akira Oosawa, Tomoyuki Sekine, Fumiko Yamada, Hidekazu Tanaka, and Masashige Matsumoto
Phys. Rev. B 77, 134420 – Published 9 April 2008

Abstract

We report the observation of the Ag-symmetric one-magnon Raman peak in the magnon Bose-Einstein condensation phase of TlCuCl3. Its Raman shift traces the one-magnon energy at the magnetic Γ point, and its intensity is proportional to the squared transverse magnetization. The appearance of the one-magnon Raman scattering originates from the exchange magnon Raman process and reflects the change of the magnetic-state symmetry. By using the bond-operator representation, we theoretically clarify the Raman selection rules, which are consistent with the experimental results.

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  • Received 2 January 2008
  • Corrected 10 April 2008

DOI:https://doi.org/10.1103/PhysRevB.77.134420

©2008 American Physical Society

Corrections

10 April 2008

Erratum

Publisher's Note: Magnetic field induced one-magnon Raman scattering in the magnon Bose-Einstein condensation phase of TlCuCl3 [Phys. Rev. B 77, 134420 (2008)]

Haruhiko Kuroe, Kouhei Kusakabe, Akira Oosawa, Tomoyuki Sekine, Fumiko Yamada, Hidekazu Tanaka, and Masashige Matsumoto
Phys. Rev. B 77, 139905 (2008)

Authors & Affiliations

Haruhiko Kuroe*, Kouhei Kusakabe, Akira Oosawa, and Tomoyuki Sekine

  • Department of Physics, Sophia University, 7-1 Kioi-cho, Chiyoda-ku, Tokyo 102-8554, Japan

Fumiko Yamada and Hidekazu Tanaka

  • Department of Physics, Tokyo Institute of Technology, Oh-okayama, Meguro-ku, Tokyo 152-8551, Japan

Masashige Matsumoto

  • Department of Physics, Shizuoka University, 836 Oya, Shizuoka 422-8529, Japan

  • *kuroe@sophia.ac.jp

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Issue

Vol. 77, Iss. 13 — 1 April 2008

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