TY - JOUR
T1 - Evolution of magnetism in single-crystal Ca2 Ru1-xI rxO4 (0≤x≤0.65)
AU - Yuan, S. J.
AU - Terzic, J.
AU - Wang, J. C.
AU - Li, L.
AU - Aswartham, S.
AU - Song, W. H.
AU - Ye, F.
AU - Cao, G.
N1 - Publisher Copyright:
© 2015 American Physical Society. ©2015 American Physical Society.
PY - 2015/7/24
Y1 - 2015/7/24
N2 - We report structural, magnetic, transport, and thermal properties of single-crystal Ca2 Ru1-xI rxO4 (0≤x≤0.65). Ca2RuO4 is a structurally driven Mott insulator with a metal-insulator transition at TMI=357K, which is well separated from antiferromagnetic order at TN=110K. Substitution of a 5d element, Ir, for Ru enhances spin-orbit coupling and locking between the structural distortions and magnetic moment canting. Ir doping intensifies the distortion or rotation of Ru/IrO6 octahedra and induces weak ferromagnetic behavior along the c axis. In particular, Ir doping suppresses TN but concurrently causes an additional magnetic ordering TN2 at a higher temperature up to 210 K for x=0.65. The effect of Ir doping sharply contrasts with that of 3d-element doping such as Cr, Mn, and Fe, which suppresses TN and induces unusual negative volume thermal expansion. The stark difference between 3d- and 5d-element doping underlines a strong magnetoelastic coupling inherent in the Ir-rich oxides.
AB - We report structural, magnetic, transport, and thermal properties of single-crystal Ca2 Ru1-xI rxO4 (0≤x≤0.65). Ca2RuO4 is a structurally driven Mott insulator with a metal-insulator transition at TMI=357K, which is well separated from antiferromagnetic order at TN=110K. Substitution of a 5d element, Ir, for Ru enhances spin-orbit coupling and locking between the structural distortions and magnetic moment canting. Ir doping intensifies the distortion or rotation of Ru/IrO6 octahedra and induces weak ferromagnetic behavior along the c axis. In particular, Ir doping suppresses TN but concurrently causes an additional magnetic ordering TN2 at a higher temperature up to 210 K for x=0.65. The effect of Ir doping sharply contrasts with that of 3d-element doping such as Cr, Mn, and Fe, which suppresses TN and induces unusual negative volume thermal expansion. The stark difference between 3d- and 5d-element doping underlines a strong magnetoelastic coupling inherent in the Ir-rich oxides.
UR - http://www.scopus.com/inward/record.url?scp=84938906994&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.92.024425
DO - 10.1103/PhysRevB.92.024425
M3 - Article
AN - SCOPUS:84938906994
SN - 1098-0121
VL - 92
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 2
M1 - 024425
ER -