TY - JOUR
T1 - Characteristic crossing point (T* ≈ 2.7K) in specific heat curves of samples RuSr2Gd1.5Ce0.5Cu 2O10-δ taken for different values of magnetic field
AU - Belevtsev, B. I.
AU - Krasovitsky, V. B.
AU - Naugle, D. G.
AU - Rathnayaka, K. D.D.
AU - Agnolet, G.
AU - Felner, I.
PY - 2009
Y1 - 2009
N2 - Magnetic properties of polycrystalline samples of RuSr2(Gd 1.5Ce0.5)Cu2O10-δ, as-prepared (by solid-state reaction) and annealed (12h at 845 °C) in pure oxygen at different pressure (30, 62 and 78atm) are presented. The specific heat and magnetization were investigated in the temperature range 1.8-300K with a magnetic field up to 8T. The specific heat, C(T), shows a jump at the superconducting transition (with an onset at T≈37.5K). Below 20K, a Schottky-type anomaly becomes apparent in C(T). This low-temperature anomaly can be attributed to splitting of the ground term 8S7/2 of paramagnetic Gd3+ ions by internal and external magnetic fields. It is found that curves C(T) taken for different values of magnetic field have the same crossing point (at T*≈2.7K) for all the samples studied. At the same time, C(H) curves taken for different temperatures have a crossing point at a characteristic field H*≈3.7T. These effects can be considered as a manifestation of the crossing point phenomenon which is supposed to be inherent for strongly correlated electron systems.
AB - Magnetic properties of polycrystalline samples of RuSr2(Gd 1.5Ce0.5)Cu2O10-δ, as-prepared (by solid-state reaction) and annealed (12h at 845 °C) in pure oxygen at different pressure (30, 62 and 78atm) are presented. The specific heat and magnetization were investigated in the temperature range 1.8-300K with a magnetic field up to 8T. The specific heat, C(T), shows a jump at the superconducting transition (with an onset at T≈37.5K). Below 20K, a Schottky-type anomaly becomes apparent in C(T). This low-temperature anomaly can be attributed to splitting of the ground term 8S7/2 of paramagnetic Gd3+ ions by internal and external magnetic fields. It is found that curves C(T) taken for different values of magnetic field have the same crossing point (at T*≈2.7K) for all the samples studied. At the same time, C(H) curves taken for different temperatures have a crossing point at a characteristic field H*≈3.7T. These effects can be considered as a manifestation of the crossing point phenomenon which is supposed to be inherent for strongly correlated electron systems.
UR - http://www.scopus.com/inward/record.url?scp=73049085715&partnerID=8YFLogxK
U2 - 10.1088/0953-8984/21/45/455602
DO - 10.1088/0953-8984/21/45/455602
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AN - SCOPUS:73049085715
SN - 0953-8984
VL - 21
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 45
M1 - 455602
ER -