TY - JOUR
T1 - Anomalous positive magnetoresistance in Fe0.75 Mn1.35 As
AU - Sun, N. K.
AU - Li, Y. B.
AU - Li, D.
AU - Zhang, Q.
AU - Feng, W. J.
AU - Zhang, Z. D.
PY - 2006
Y1 - 2006
N2 - With increasing temperature, tetragonal Fe0.75 Mn1.35 As compound exhibits a first-order phase transition at Ts =165 K from a ferrimagnetic (FI) phase with a large unit-cell volume to an antiferromagnetic (AF) phase with a small unit-cell volume. An external magnetic field induces a metamagnetic transition from the AF to the FI state above Ts, stabilizing the phase with the larger cell volume. With increasing the number of warming and cooling cycles, the resistivity curve, ρ(T), shifts to higher values, and this shift is ascribed to a pronounced reduction of the mean-free path of electron scattering. After several thermocycles, a large, irreversible lattice expansion of c axis of 0.18% occurs. The positive magnetoresistance ratios as large as 12% and 6% for the first magnetic-field cycles are observed at 170 and 167 K, respectively, at 5 T. The overall magnetotransport behaviors on the subsequently second and third magnetic-field cycles at 170 K are similar to that in the first magnetic-field cycle, but with MR ratios of only 1.6% and 0.6%, respectively, at 5 T.
AB - With increasing temperature, tetragonal Fe0.75 Mn1.35 As compound exhibits a first-order phase transition at Ts =165 K from a ferrimagnetic (FI) phase with a large unit-cell volume to an antiferromagnetic (AF) phase with a small unit-cell volume. An external magnetic field induces a metamagnetic transition from the AF to the FI state above Ts, stabilizing the phase with the larger cell volume. With increasing the number of warming and cooling cycles, the resistivity curve, ρ(T), shifts to higher values, and this shift is ascribed to a pronounced reduction of the mean-free path of electron scattering. After several thermocycles, a large, irreversible lattice expansion of c axis of 0.18% occurs. The positive magnetoresistance ratios as large as 12% and 6% for the first magnetic-field cycles are observed at 170 and 167 K, respectively, at 5 T. The overall magnetotransport behaviors on the subsequently second and third magnetic-field cycles at 170 K are similar to that in the first magnetic-field cycle, but with MR ratios of only 1.6% and 0.6%, respectively, at 5 T.
UR - http://www.scopus.com/inward/record.url?scp=33750604767&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.74.172402
DO - 10.1103/PhysRevB.74.172402
M3 - Article
AN - SCOPUS:33750604767
SN - 1098-0121
VL - 74
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 17
M1 - 172402
ER -