Material Specification for Sm:123; [Sm-Ba-Cu-O]
Process: Pyrolysis
Notes: The authors cite Z. Bukowski et al., in Superconductivity, Proc. ICMAS '92, Paris, 21-22 October 1992, eds. C.W. Chu and J. Fink (IITT-International, Gournay-sur-Marne, 1992) and summarize the procedure as follows. "Two series of Sm1+xBa2-xCu3Oy ceramic samples were prepared by the citrate pyrolysis process... The first, Sm1+xBa2-xCu3O
, is a series of solid solutions with maximum oxygen content, y
, which can be achieved in the common oxygenation procedure. The second, Sm1Ba2Cu3Oy, is a series of samples with exact 123 stoichiometry and different oxygen contents."
Formula: Sm1+xBa2-xCu3Oy
Informal Name: Sm:123
Chemical Family: Sm-Ba-Cu-O
Chemical Class: Oxide
Structure Type: Polycrystalline
Manufacturer: In House
Commercial Name: In House
Production Date:
Lot Number:
Production Form:
Critical Temperature for Sm:123; [Sm-Ba-Cu-O]
x of Sm1+x (formula units) |
y of Oy (formula units) |
Critical Temperature (K) |
0 |
6.85 |
90.4 |
0 |
6.73 |
45 |
0 |
6.11 |
0 |
0.27 |
7.05 |
50 |
0.6 |
7.11 |
0 |
Measurement Method: Four-probe method
"The resistivity ... was measured by a standard four-point method and the... curves were used to determine the critical temperature... as a midpoint of the superconducting transition." No additional measurement details were noted.
Cautions: Unevaluated Data
Resistivity (normal state) for Sm:123; [Sm-Ba-Cu-O]
x of Sm1+x (formula units) |
y of Oy (formula units) |
Temperature (K) |
Resistivity (normal state) (mΩ·cm) |
0 |
6.62 |
26 |
0.01 |
0 |
6.62 |
32 |
1.68 |
0 |
6.62 |
35 |
4.69 |
0 |
6.62 |
38 |
6.38 |
0 |
6.62 |
44 |
7.99 |
0 |
6.62 |
67 |
6.88 |
0 |
6.62 |
113 |
5.26 |
0 |
6.62 |
152 |
4.95 |
0 |
6.62 |
203 |
5.45 |
0 |
6.62 |
250 |
6.25 |
0 |
6.62 |
292 |
6.90 |
0 |
6.73 |
36 |
0.06 |
0 |
6.73 |
41 |
0.01 |
0 |
6.73 |
44 |
1.38 |
0 |
6.73 |
47 |
2.26 |
0 |
6.73 |
53 |
3.80 |
0 |
6.73 |
74 |
3.36 |
0 |
6.73 |
99 |
3.06 |
0 |
6.73 |
123 |
2.98 |
0 |
6.73 |
148 |
3.12 |
0 |
6.73 |
190 |
3.47 |
0 |
6.73 |
237 |
4.05 |
0 |
6.73 |
294 |
4.55 |
0 |
6.82 |
60 |
0.06 |
0 |
6.82 |
60 |
0.79 |
0 |
6.82 |
68 |
1.30 |
0 |
6.82 |
86 |
1.52 |
0 |
6.82 |
127 |
1.73 |
0 |
6.82 |
166 |
2.01 |
0 |
6.82 |
205 |
2.30 |
0 |
6.82 |
244 |
2.51 |
0 |
6.82 |
293 |
2.79 |
0 |
6.85 |
91 |
0.05 |
0 |
6.85 |
93 |
0.49 |
0 |
6.85 |
114 |
0.63 |
0 |
6.85 |
158 |
0.84 |
0 |
6.85 |
205 |
0.97 |
0 |
6.85 |
254 |
1.18 |
0 |
6.85 |
298 |
1.24 |
0.45 |
0.09 |
20 |
258 |
0.45 |
0.09 |
35 |
140 |
0.45 |
0.09 |
60 |
78 |
0.45 |
0.09 |
115 |
26 |
0.45 |
0.09 |
162 |
19 |
0.45 |
0.09 |
204 |
12 |
0.45 |
0.09 |
253 |
4.8 |
0.45 |
0.09 |
295 |
1.6 |
0.60 |
7.11 |
75 |
1000 |
0.60 |
7.11 |
85 |
784 |
0.60 |
7.11 |
102 |
492 |
0.60 |
7.11 |
124 |
285 |
0.60 |
7.11 |
150 |
151 |
0.60 |
7.11 |
191 |
87 |
0.60 |
7.11 |
230 |
52 |
0.60 |
7.11 |
269 |
31 |
0.60 |
7.11 |
292 |
28 |
0.39 |
7.07 |
26 |
0.00 |
0.39 |
7.07 |
31 |
2.19 |
0.39 |
7.07 |
32 |
5.09 |
0.39 |
7.07 |
35 |
6.90 |
0.39 |
7.07 |
40 |
8.23 |
0.39 |
7.07 |
63 |
6.97 |
0.39 |
7.07 |
102 |
5.55 |
0.39 |
7.07 |
153 |
4.84 |
0.39 |
7.07 |
213 |
4.99 |
0.39 |
7.07 |
257 |
5.22 |
0.39 |
7.07 |
293 |
5.45 |
0.27 |
7.05 |
49 |
0.00 |
0.27 |
7.05 |
52 |
1.09 |
0.27 |
7.05 |
57 |
2.11 |
0.27 |
7.05 |
91 |
2.18 |
0.27 |
7.05 |
143 |
2.33 |
0.27 |
7.05 |
189 |
2.56 |
0.27 |
7.05 |
236 |
2.79 |
0.27 |
7.05 |
290 |
3.02 |
0.27 |
7.05 |
295 |
3.01 |
0.15 |
6.99 |
83 |
0.00 |
0.15 |
6.99 |
85 |
0.54 |
0.15 |
6.99 |
91 |
0.85 |
0.15 |
6.99 |
124 |
1.08 |
0.15 |
6.99 |
173 |
1.31 |
0.15 |
6.99 |
215 |
1.46 |
0.15 |
6.99 |
254 |
1.61 |
0.15 |
6.99 |
293 |
1.68 |
Measurement Method: Four-probe method
"The resistivity ... was measured by a standard four-point method and the... curves were used to determine the critical temperature... as a midpoint of the superconducting transition." No additional measurement details were noted.
Cautions: Unevaluated Data
Digitized data were obtained from Figures 3 and 4 of the paper.
Specific Heat for Sm:123; [Sm-Ba-Cu-O]
x of Sm1+x (formula units) |
y of Oy (formula units) |
Temperature (K) |
Specific Heat (J kg-1 K-1) |
0 |
6.85 |
63 |
9.5 |
0 |
6.85 |
106 |
16.6 |
0 |
6.85 |
150 |
22.1 |
0 |
6.85 |
193 |
25.8 |
0 |
6.85 |
249 |
29.2 |
0 |
6.85 |
300 |
31.0 |
0 |
6.73 |
94 |
15.1 |
0 |
6.73 |
137 |
21.0 |
0 |
6.73 |
169 |
24.0 |
0 |
6.73 |
213 |
27.2 |
0 |
6.73 |
254 |
29.3 |
0 |
6.73 |
297 |
30.8 |
0 |
6.11 |
86 |
14.9 |
0 |
6.11 |
128 |
20.3 |
0 |
6.11 |
169 |
24.3 |
0 |
6.11 |
215 |
28.1 |
0 |
6.11 |
254 |
29.7 |
0 |
6.11 |
297 |
31.2 |
0.27 |
7.05 |
84 |
13.1 |
0.27 |
7.05 |
129 |
19.7 |
0.27 |
7.05 |
194 |
26.2 |
0.27 |
7.05 |
264 |
30.7 |
0.6 |
7.11 |
86 |
13.0 |
0.6 |
7.11 |
129 |
19.1 |
0.6 |
7.11 |
175 |
23.6 |
0.6 |
7.11 |
221 |
27.1 |
0.6 |
7.1 |
269 |
29.2 |
Measurement Method: Adiabatic calorimetry
The authors cite D. Wlosewicz et al., Cryogenics, Vol. 32, 265 (1992), and summarize the procedure as follows. "The specific heat measurements were carried out in the automated adiabatic calorimeter... The calorimeter operation alternately combines two different modes: a heat pulse method with better absolute accuracy and a faster continuous method with better resolution. The typical heating rate for both methods is 5-10 mK/s. The sample mass varied around 300 mg, which was sufficiently small to achieve a satisfactorily short time for thermal equilibrium (below 60 s) for the used heating rates. At least two pieces of each sample were investigated showing variations smaller than 1.5% and the results were averaged."
Cautions: Evaluated Data
Digitized data were obtained from Figure 5 of the paper.
Debye Temperature for Sm:123; [Sm-Ba-Cu-O]
x of Sm1+x (formula units) |
y of Oy (formula units) |
Temperature (K) |
Debye Temperature (K) |
0 |
6.85 |
69 |
389 |
0 |
6.85 |
94 |
431 |
0 |
6.85 |
121 |
460 |
0 |
6.85 |
147 |
477 |
0 |
6.85 |
172 |
487 |
0 |
6.85 |
198 |
493 |
0 |
6.85 |
222 |
495 |
0 |
6.85 |
247 |
493 |
0 |
6.85 |
271 |
493 |
0 |
6.85 |
298 |
499 |
0 |
6.73 |
80 |
409 |
0 |
6.73 |
100 |
432 |
0 |
6.73 |
120 |
451 |
0 |
6.73 |
139 |
466 |
0 |
6.73 |
157 |
476 |
0 |
6.73 |
192 |
484 |
0 |
6.73 |
230 |
487 |
0 |
6.73 |
247 |
487 |
0 |
6.73 |
271 |
486 |
0 |
6.73 |
291 |
487 |
0 |
6.11 |
82 |
390 |
0 |
6.11 |
100 |
418 |
0 |
6.11 |
120 |
441 |
0 |
6.11 |
141 |
458 |
0 |
6.11 |
180 |
480 |
0 |
6.11 |
218 |
487 |
0 |
6.11 |
261 |
486 |
0 |
6.11 |
279 |
484 |
0 |
6.11 |
300 |
489 |
0.27 |
7.05 |
69 |
396 |
0.27 |
7.05 |
94 |
437 |
0.27 |
7.05 |
121 |
466 |
0.27 |
7.05 |
147 |
485 |
0.27 |
7.05 |
174 |
493 |
0.27 |
7.05 |
200 |
496 |
0.27 |
7.05 |
226 |
495 |
0.27 |
7.05 |
251 |
493 |
0.27 |
7.05 |
277 |
493 |
0.27 |
7.05 |
304 |
491 |
0.6 |
7.11 |
82 |
419 |
0.6 |
7.11 |
100 |
448 |
0.6 |
7.11 |
121 |
469 |
0.6 |
7.11 |
139 |
485 |
0.6 |
7.11 |
159 |
498 |
0.6 |
7.11 |
178 |
506 |
0.6 |
7.11 |
198 |
512 |
0.6 |
7.11 |
237 |
518 |
0.6 |
7.11 |
275 |
516 |
0.6 |
7.11 |
296 |
518 |
Measurement Method: Adiabatic calorimetry
The authors cite D. Wlosewicz et al., Cryogenics, Vol. 32, 265 (1992), and summarize the procedure as follows. "The specific heat measurements were carried out in the automated adiabatic calorimeter... The calorimeter operation alternately combines two different modes: a heat pulse method with better absolute accuracy and a faster continuous method with better resolution. The typical heating rate for both methods is 5-10 mK/s. The sample mass varied around 300 mg, which was sufficiently small to achieve a satisfactorily short time for thermal equilibrium (below 60 s) for the used heating rates. At least two pieces of each sample were investigated showing variations smaller than 1.5% and the results were averaged."
Cautions: Evaluated Data
Digitized data were obtained from Figure 7 of the paper.