TY - JOUR
T1 - Thermal conductivity in the stripe-ordered phase of cuprates and nickelates
AU - Yan, J. Q.
AU - Zhou, J. S.
AU - Goodenough, B.
PY - 2003
Y1 - 2003
N2 - The temperature dependence of the thermal conductivity κ and the resistivity ρ have been measured on well-characterized crystals La1.60-xNd0.4SrxCuO4 (x=0.12, 0.15, and 0.20), La2CuO4+δ, and La2-xSrxNiO4 (x=0, 0.33, 0.50). In La2CuO4+δ, the phonon component of κ(T) decreases sharply with increasing δ. The charge ordering at TCO in La1.67Sr0.33NiO4 enhances κ(T). Similarly in the La1.60-xNd0.4SrxCuO4 system, ordering of the mobile holes into stripes within the CuO2 sheets on cooling through a low-temperature tetragonal/orthorhombic (LTT/LTO) transition at Tt gives a jump Δκ in κ(T). In contrast to a previous report on ceramic samples, the superconductive crystals x=0.15 and 0.20 of the La1.60-xNd0.4SrxCuO4 system show a clear low-temperature peak in the normal state κ(T) below Tt that shows phonons are the dominant carriers of heat in the LTT phase. Restoring phonons in the LTT phase is thus seen to be compatible with superconductivity in the copper oxides, albeit with a lower Tc than is found in the LTO phase where the phonon component of κ(T) is suppressed in the normal state by the bond-length fluctuations.
AB - The temperature dependence of the thermal conductivity κ and the resistivity ρ have been measured on well-characterized crystals La1.60-xNd0.4SrxCuO4 (x=0.12, 0.15, and 0.20), La2CuO4+δ, and La2-xSrxNiO4 (x=0, 0.33, 0.50). In La2CuO4+δ, the phonon component of κ(T) decreases sharply with increasing δ. The charge ordering at TCO in La1.67Sr0.33NiO4 enhances κ(T). Similarly in the La1.60-xNd0.4SrxCuO4 system, ordering of the mobile holes into stripes within the CuO2 sheets on cooling through a low-temperature tetragonal/orthorhombic (LTT/LTO) transition at Tt gives a jump Δκ in κ(T). In contrast to a previous report on ceramic samples, the superconductive crystals x=0.15 and 0.20 of the La1.60-xNd0.4SrxCuO4 system show a clear low-temperature peak in the normal state κ(T) below Tt that shows phonons are the dominant carriers of heat in the LTT phase. Restoring phonons in the LTT phase is thus seen to be compatible with superconductivity in the copper oxides, albeit with a lower Tc than is found in the LTO phase where the phonon component of κ(T) is suppressed in the normal state by the bond-length fluctuations.
UR - http://www.scopus.com/inward/record.url?scp=0142153796&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.68.104520
DO - 10.1103/PhysRevB.68.104520
M3 - Article
AN - SCOPUS:0142153796
SN - 1098-0121
VL - 68
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 10
ER -