TY - JOUR
T1 - Magnetic phase diagram of the multiferroic FeTe2O5Br
AU - Pregelj, M.
AU - Zorko, A.
AU - Zaharko, O.
AU - Kutnjak, Z.
AU - Jagodič, M.
AU - Jagličić, Z.
AU - Berger, H.
AU - De Souza, M.
AU - Balz, C.
AU - Lang, M.
AU - Arčon, D.
PY - 2010/10/27
Y1 - 2010/10/27
N2 - The low-temperature magnetic phase diagram of the multiferroic system FeTe2O5Br down to 300 mK and up to 9 T is presented. Short-range magnetic correlations within the crystal layers start to develop already at ∼50 K, i.e., far above TN1 ∼11.0 K, where the system undergoes a magnetic phase transition into the high-temperature incommensurate (HT-ICM) phase. Only 0.5 K lower, at TN2, the system undergoes a second phase transition into the low-temperature incommensurately modulated (LT-ICM) phase accompanied by a spontaneous electric polarization. When the magnetic field is applied, the transition temperatures shift depending on the field orientation. In the case of B-b and B>4.5 T, the HT-ICM phase disappears along with the electric polarization in the LT-ICM phase. The field dependence of the magnetic transition temperatures is explained in the context of the magnetic susceptibility behavior. Similarities and differences between the novel well-established magnetoelectrics are discussed.
AB - The low-temperature magnetic phase diagram of the multiferroic system FeTe2O5Br down to 300 mK and up to 9 T is presented. Short-range magnetic correlations within the crystal layers start to develop already at ∼50 K, i.e., far above TN1 ∼11.0 K, where the system undergoes a magnetic phase transition into the high-temperature incommensurate (HT-ICM) phase. Only 0.5 K lower, at TN2, the system undergoes a second phase transition into the low-temperature incommensurately modulated (LT-ICM) phase accompanied by a spontaneous electric polarization. When the magnetic field is applied, the transition temperatures shift depending on the field orientation. In the case of B-b and B>4.5 T, the HT-ICM phase disappears along with the electric polarization in the LT-ICM phase. The field dependence of the magnetic transition temperatures is explained in the context of the magnetic susceptibility behavior. Similarities and differences between the novel well-established magnetoelectrics are discussed.
UR - http://www.scopus.com/inward/record.url?scp=78049460255&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.82.144438
DO - 10.1103/PhysRevB.82.144438
M3 - Article
AN - SCOPUS:78049460255
SN - 1098-0121
VL - 82
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 14
M1 - 144438
ER -