TY - JOUR
T1 - Electrical and thermal transport properties of Dy0.95Pr 0.05Ba2(Cu1-x Mx)3O 7-δ with (M=Fe, Co, Ni and Zn) bulk superconductors
AU - Geetha, M.
AU - Rao, Ashok
AU - Thukaram, M.
AU - Agarwal, S. K.
AU - Bhatt, Ramesh Chandra
AU - Tyagi, Kriti
AU - Kuo, Y. K.
PY - 2014/6/1
Y1 - 2014/6/1
N2 - In the present communication, measurements of transition temperature, thermal conductivity, thermoelectric power and specific heat have been carried out on pristine and co-doped samples of Dy0.95Pr 0.05Ba2(Cu0.98 M0.02) 3O7-δ system [M=Fe, Co, Ni and Zn]. The electrical resistivity results show that all the samples exhibit metallic behavior. The thermal conductivity results illustrate that for pristine sample of DyBa 2Cu3O7-δ, the expected pronounced hump in thermal conductivity is seen below the transition temperature. The hump is suppressed with 5% Pr-doping and this is further suppressed with co-doping. The thermoelectric power measurements show that the pristine sample exhibits hole-like behavior and this continues for doped as well co-doped samples. Pristine sample shows the expected jump in specific heat and with Pr-doping a slope change is observed near the transition temperature.
AB - In the present communication, measurements of transition temperature, thermal conductivity, thermoelectric power and specific heat have been carried out on pristine and co-doped samples of Dy0.95Pr 0.05Ba2(Cu0.98 M0.02) 3O7-δ system [M=Fe, Co, Ni and Zn]. The electrical resistivity results show that all the samples exhibit metallic behavior. The thermal conductivity results illustrate that for pristine sample of DyBa 2Cu3O7-δ, the expected pronounced hump in thermal conductivity is seen below the transition temperature. The hump is suppressed with 5% Pr-doping and this is further suppressed with co-doping. The thermoelectric power measurements show that the pristine sample exhibits hole-like behavior and this continues for doped as well co-doped samples. Pristine sample shows the expected jump in specific heat and with Pr-doping a slope change is observed near the transition temperature.
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U2 - 10.1016/j.ssc.2014.02.007
DO - 10.1016/j.ssc.2014.02.007
M3 - Article
AN - SCOPUS:84897711838
SN - 0038-1098
VL - 187
SP - 38
EP - 42
JO - Solid State Communications
JF - Solid State Communications
ER -