SPECIFIC HEAT OF THE HIGH Tc SUPERCONDUCTOR Bi-Sr-Ca-Cu-O

1988 ◽  
Vol 02 (07) ◽  
pp. 885-889 ◽  
Author(s):  
S.L. YUAN ◽  
J.W. LI ◽  
W. WANG ◽  
Q.Z. RAN ◽  
G.G. ZHENG ◽  
...  

The Bi-Sr-Ca-Cu-O superconductor with the nominal composition (1113) were prepared. An orthorhombic unit cell (a=0.544 nm , b=0.543 nm , c=3.07 nm ) was determined by X-ray diffraction. The resistance transition curve shows that the sample has an onset around 110K and the zero resistance temperature at 85K. The mutual inductance measurement also shows a two-step transition which correspond to two superconducting phases as well as that in the resistive transition. The specific heat measurement was performed in the range of 56K to 130K by continuous scanning method. A simple extrapolation of the curve was made both from below and above T c to yield ΔC=45 mj /g. K and ΔC/T c =0.49 mj /g. K 2. From these values, the Sommerfeld constant γ and the Debye temperature θ D were estimated.

1988 ◽  
Vol 02 (03n04) ◽  
pp. 421-425 ◽  
Author(s):  
S. L. YUAN ◽  
J. W. LI ◽  
W. WANG ◽  
Q. Z. RAN ◽  
G. G. ZHENG ◽  
...  

The Bi-Sr-Ca-Cu-O superconductors with the nominal composition (1113) were prepared. An orthorhombic unit cell (a = 0.544 nm , b = 0.543 nm , c = 3.07 nm ) was determined by X-ray diffraction. The resistance transition curve shows that the sample has an onset around 110 K and the zero resistance temperature at 85 K. The mutual inductance measurement also shows a two-step transition which correspond to two superconducting phases as well as that in the resistive transition. The specific heat measurement was performed in the range of 56 K to 130 K by the continuous scanning method. A simple extrapolation of the curve was made from below and from above Tc to yield ΔC = 45 mJ/g.K and ΔC/Tc = 0.49 mJ/g.K .2 From these values, the Sommerfeld constant γ and the Debye temperature θ D were estimated.


2018 ◽  
Vol 87 (9) ◽  
pp. 093703 ◽  
Author(s):  
Shunichiro Kittaka ◽  
Shota Nakamura ◽  
Toshiro Sakakibara ◽  
Naoki Kikugawa ◽  
Taichi Terashima ◽  
...  

2012 ◽  
Vol 81 (12) ◽  
pp. 125002 ◽  
Author(s):  
Hiroshi Takatsu ◽  
Yoshikazu Mizuguchi ◽  
Hiroki Izawa ◽  
Osuke Miura ◽  
Hiroaki Kadowaki

1975 ◽  
Vol 28 (1) ◽  
pp. K77-K80 ◽  
Author(s):  
V. Franke ◽  
E. Hegenbarth ◽  
B. Březina

2006 ◽  
Vol 383 (1) ◽  
pp. 67-70 ◽  
Author(s):  
Y. Taguchi ◽  
A. Kitora ◽  
M. Hisakabe ◽  
Y. Iwasa

1990 ◽  
Vol 04 (04) ◽  
pp. 293-299
Author(s):  
YUGUI WANG ◽  
JINSONG WANG ◽  
NANLIN WANG ◽  
XINPING JIAO ◽  
GUCHANG HAN ◽  
...  

The resistance and ac susceptibility measurements show that cooling rate of the cast-annealing samples in heat treatment process has some effect on the 110 K superconducting phase in Bi–Pb–Sr–Ca–Cu–O system. Rapid quenching of the sample in air from 845°C causes oxygen deficiency in lattice and brings about a trifling change of unit cell size along c-axis direction. The dc magnetization and specific heat anomaly ∆c measurements demonstrate that fast cooling rate can reduce the transition temperature of high T c phase and the lower critical field, and weaken the pinning forces for vertex lines. The peak value of specific heat anomaly of the sample with nominal composition of Bi 1.7 Pb 0.3 Sr 2 Ca 2 Cu 4.5 O y is still small in comparison with YBa 2 Cu 3 O 7. From the magnetization curve we can estimate that the superconducting volume fraction is about 20%.


1989 ◽  
Vol 03 (01) ◽  
pp. 15-23 ◽  
Author(s):  
P.T. WU ◽  
R.S. LIU ◽  
J.M. LIANG ◽  
Y.T. HUANG ◽  
L.J. CHEN

The process leading to the discovery of possible superconductivity with zero resistance up to 162 K for multiphase samples with nominal composition TlCa 4 Ba 3 Cu 6 O x is briefly reviewed. The discovery was made during the deliberate course to fabricate superconducting compounds with more than three Cu-O layers interposed between Tl-O layers.


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