TY - JOUR
T1 - Nature of the specific heat anomaly in the Bi and Tl high temperature superconductors
AU - Seidler, F.
AU - Böhm, P.
AU - Geus, H.
AU - Braunisch, W.
AU - Braun, E.
AU - Schnelle, W.
AU - Drzazga, Z.
AU - Wild, N.
AU - Roden, B.
AU - Schmidt, H.
AU - Wohlleben, D.
AU - Felner, I.
AU - Wolfus, Y.
PY - 1989/3/1
Y1 - 1989/3/1
N2 - Specific heat, field cooling Meissner effect, isothermal magnetization, AC susceptibility and resistance were measured on sintered pellets of the Bi and Tl high temperature superconductors with nominal compositions BiPb0.3SrCaCu2O5.8 and Tl2Ba2CaCu2O8, and for comparison on some pellets of the REBa2Cu3O6.9 system. With decreasing field, the field cooling Meissner signals of the Bi and Tl systems approach the same magnitude and transition width (ΔT ≈ 2-3 K) as in high quality pellets of the REBa2Cu3O6.9. The field and temperature dependence of the Meissner signals is analysed in detail. At the transition temperatures of five superconducting phases of the Bi and Tl pellets, the specific heat shows no jumps nor maxima, within the accuracy of the measurement (Δ(C/T) < mJ/(mol K2)). There are however sharp breaks of the slope of C/T at the Tc values, which are intrinsically as large as in the REBa2Cu3O6.9. The transitions in the Bi and Tl systems look more like third order transitions rather than like the second order transitions of the REBa2Cu3O6.9.
AB - Specific heat, field cooling Meissner effect, isothermal magnetization, AC susceptibility and resistance were measured on sintered pellets of the Bi and Tl high temperature superconductors with nominal compositions BiPb0.3SrCaCu2O5.8 and Tl2Ba2CaCu2O8, and for comparison on some pellets of the REBa2Cu3O6.9 system. With decreasing field, the field cooling Meissner signals of the Bi and Tl systems approach the same magnitude and transition width (ΔT ≈ 2-3 K) as in high quality pellets of the REBa2Cu3O6.9. The field and temperature dependence of the Meissner signals is analysed in detail. At the transition temperatures of five superconducting phases of the Bi and Tl pellets, the specific heat shows no jumps nor maxima, within the accuracy of the measurement (Δ(C/T) < mJ/(mol K2)). There are however sharp breaks of the slope of C/T at the Tc values, which are intrinsically as large as in the REBa2Cu3O6.9. The transitions in the Bi and Tl systems look more like third order transitions rather than like the second order transitions of the REBa2Cu3O6.9.
UR - http://www.scopus.com/inward/record.url?scp=0024621271&partnerID=8YFLogxK
U2 - 10.1016/0921-4534(89)90262-1
DO - 10.1016/0921-4534(89)90262-1
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AN - SCOPUS:0024621271
SN - 0921-4534
VL - 157
SP - 375
EP - 394
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - 3
ER -