TY - JOUR
T1 - Magnetization study of RuSr2Y1.5Ce0.5Cu2O10
AU - Felner, I.
AU - Awana, S.
AU - Awana, S.
AU - Takayama-Muromachi, E.
PY - 2003
Y1 - 2003
N2 - We have studied the magnetic properties of nonsuperconducting RuSr2Y1.5Ce0.5Cu2O10 [L=Y, Dy, and Ho (Ru-1222)] compounds synthesized under high pressure (6 Gpa) at elevated temperature. These materials become magnetically ordered at TM=152(2) K regardless of L. The wide ferromagneticlike hysteresis loops, which open at 5 K, close themselves around Tirr=90–100 K and the remanent magnetizations (Mrem) and coercive fields (HC) become zero. Surprisingly, at Tirrrem and HC (with a peak at 120–130 K) is observed for all three samples studied. For the nonmagnetic L=Y compound, the extracted ferromagnetic moment is at 5 K and the effective paramagnetic moments are 0.75 and 2.05μB/Ru, values which are close to the expected 1μB and 1.73μB, respectively, for the low-spin state of Ru5+. We argue that the Ru-1222 system becomes: (i) antiferromagnetically ordered at TM and in this range a metamagnetic transition is induced by the external field. (ii) At TirrM, weak ferromagnetism is induced by the canting of the Ru moments.
AB - We have studied the magnetic properties of nonsuperconducting RuSr2Y1.5Ce0.5Cu2O10 [L=Y, Dy, and Ho (Ru-1222)] compounds synthesized under high pressure (6 Gpa) at elevated temperature. These materials become magnetically ordered at TM=152(2) K regardless of L. The wide ferromagneticlike hysteresis loops, which open at 5 K, close themselves around Tirr=90–100 K and the remanent magnetizations (Mrem) and coercive fields (HC) become zero. Surprisingly, at Tirrrem and HC (with a peak at 120–130 K) is observed for all three samples studied. For the nonmagnetic L=Y compound, the extracted ferromagnetic moment is at 5 K and the effective paramagnetic moments are 0.75 and 2.05μB/Ru, values which are close to the expected 1μB and 1.73μB, respectively, for the low-spin state of Ru5+. We argue that the Ru-1222 system becomes: (i) antiferromagnetically ordered at TM and in this range a metamagnetic transition is induced by the external field. (ii) At TirrM, weak ferromagnetism is induced by the canting of the Ru moments.
UR - http://www.scopus.com/inward/record.url?scp=16344378537&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.68.094508
DO - 10.1103/PhysRevB.68.094508
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
AN - SCOPUS:16344378537
SN - 1098-0121
VL - 68
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 9
ER -