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Phys. Rev. B 78, 104414 (2008) [9 pages]

Electrically driven spin excitation in the ferroelectric magnet DyMnO3

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N. Kida1, Y. Ikebe2, Y. Takahashi1, J. P. He1, Y. Kaneko1, Y. Yamasaki3, R. Shimano1,2, T. Arima4, N. Nagaosa3,5, and Y. Tokura1,3,5
1Multiferroics Project (MF), ERATO, Japan Science and Technology Agency (JST), c/o Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan
2Department of Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
3Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan
4Institute of Multidisciplinary Research for Advanced Materials, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-8577, Japan
5Cross-Correlated Materials Research Group (CMRG), ASI, RIKEN, 2-1 Hirosawa, Wako, 351-0198, Japan

Received 4 July 2008; published 18 September 2008

See accompanying Physics Synopsis

Temperature (5–250 K) and magnetic-field (0–70 kOe) variations of the low-energy (1–10 meV) electrodynamics of spin excitations have been investigated for a complete set of light-polarization configurations for a ferroelectric magnet DyMnO3 by using terahertz time-domain spectroscopy. We identify the pronounced absorption continuum (1–8 meV) with a peak feature around 2 meV, which is electric-dipole active only for the light E vector along the a axis. This absorption band grows in intensity with lowering temperature from the spin-collinear paraelectric phase above the ferroelectric transition but is independent of the orientation of spiral spin plane (bc or ab), as shown on the original Ps (ferroelectric polarization) c phase as well as the magnetic-field induced Psa phase. The possible origin of this electric-dipole active band is argued in terms of the large fluctuations of spins and spin current.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.78.104414
DOI:
10.1103/PhysRevB.78.104414
PACS:
75.80.+q, 67.30.hj, 75.40.Gb, 76.50.+g