TY - JOUR
T1 - Magnetic phase diagrams of the Kagomé staircase compound Co3 V2 O8
AU - Yen, F.
AU - Chaudhury, R. P.
AU - Galstyan, E.
AU - Lorenz, B.
AU - Wang, Y. Q.
AU - Sun, Y. Y.
AU - Chu, C. W.
N1 - Copyright:
Copyright 2008 Elsevier B.V., All rights reserved.
PY - 2008/4/1
Y1 - 2008/4/1
N2 - At zero magnetic field, a series of five phase transitions occur in Co3 V2 O8. The Néel temperature, TN = 11.4 K, is followed by four additional phase changes at T1 = 8.9 K, T2 = 7.0 K, T3 = 6.9 K, and T4 = 6.2 K. The different phases are distinguished by the commensurability of the b-component of its spin density wave vector. We investigate the stability of these various phases under magnetic fields through dielectric constant and magnetic susceptibility anomalies. The field-temperature phase diagram of Co3 V2 O8 is completely resolved. The complexity of the phase diagram results from the competition of different magnetic states with almost equal ground state energies due to competing exchange interactions and frustration.
AB - At zero magnetic field, a series of five phase transitions occur in Co3 V2 O8. The Néel temperature, TN = 11.4 K, is followed by four additional phase changes at T1 = 8.9 K, T2 = 7.0 K, T3 = 6.9 K, and T4 = 6.2 K. The different phases are distinguished by the commensurability of the b-component of its spin density wave vector. We investigate the stability of these various phases under magnetic fields through dielectric constant and magnetic susceptibility anomalies. The field-temperature phase diagram of Co3 V2 O8 is completely resolved. The complexity of the phase diagram results from the competition of different magnetic states with almost equal ground state energies due to competing exchange interactions and frustration.
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U2 - 10.1016/j.physb.2007.10.334
DO - 10.1016/j.physb.2007.10.334
M3 - Article
AN - SCOPUS:39849088435
SN - 0921-4526
VL - 403
SP - 1487
EP - 1489
JO - Physica B: Condensed Matter
JF - Physica B: Condensed Matter
IS - 5-9
ER -