Dependence of the low-temperature specific heat of YBa2Cu3O7?? on ? and magnetic field: The H1/2T term for H?0; absence of evidence for a T2 term for H=0

1996 ◽  
Vol 105 (3-4) ◽  
pp. 897-902 ◽  
Author(s):  
D. A. Wright ◽  
J. P. Emerson ◽  
B. F. Woodfield ◽  
S. F. Reklis ◽  
J. E. Gordon ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Low Temperature ◽  
Specific Heat ◽  
Low Temperature Specific Heat ◽  
Absence Of Evidence

Dependence of the low-temperature specific heat of YBa2Cu3O7?? on ? and magnetic field: Concentrations of spin-2 and spin-1/2 paramagnetic centers

1996 ◽  
Vol 105 (3-4) ◽  
pp. 891-896 ◽  
Author(s):  
J. P. Emerson ◽  
D. A. Wright ◽  
B. F. Woodfield ◽  
J. E. Gordon ◽  
R. A. Fisher ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Low Temperature ◽  
Specific Heat ◽  
Paramagnetic Centers ◽  
Low Temperature Specific Heat

Low-Temperature Specific Heat in High Magnetic Field of Bi 2 Sr 2 CaCu 2 O 8

1989 ◽  
Vol 8 (7) ◽  
pp. 639-643 ◽  
Author(s):  
R Caspary ◽  
A Höhr ◽  
H Spille ◽  
F Steglich ◽  
H Schmidt ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Low Temperature ◽  
Specific Heat ◽  
High Magnetic Field ◽  
Low Temperature Specific Heat

THE LOW-TEMPERATURE SPECIFIC HEAT OF U(Pt, Pd)3

1993 ◽  
Vol 07 (01n03) ◽  
pp. 14-17
Author(s):  
H. P. VAN DER MEULEN ◽  
J. J. M. FRANSE ◽  
A. DE VISSER
Keyword(s):  
Magnetic Field ◽  
Low Temperature ◽  
Specific Heat ◽  
Applied Magnetic Field ◽  
Low Temperatures ◽  
Single Crystalline ◽  
Normal Part ◽  
Electron Contribution ◽  
Heavy Electron ◽  
Low Temperature Specific Heat

Specific-heat measurements on single-crystalline samples of U ( Pt 1− x Pd x )3 ( x = 0.00, 0.05 and 0.10) reveal anomalously large values for c/T at low temperatures. The data for UPt 3 have previously been analyzed by making use of the enhanced value of the low-temperature Grüneisen parameter. By this analysis, the heavy-electron contribution to the specific heat has been separated from the normal part that is largely due to the phonon term. Taking this latter term to be the same for all three compounds, the heavy-electron contribution has been evaluated for temperatures below 20 K. This contribution is compared with a spin-1/2 Kondo-type of specific heat. The resulting curves for the x = 0.00 and x = 0.10 alloys are very similar and mainly differ in the temperature at which the maximum is found. The effect of an applied magnetic field within the hexagonal plane, however, shifts the maximum to lower temperatures for x = 0.00 whereas for x = 0.10 a shift towards higher temperatures is found.

Magnetic-field dependence of the low-temperature specific heat ofLa2−xSrxCuO4

1998 ◽  
Vol 58 (22) ◽  
pp. R14753-R14756 ◽  
Author(s):  
S. J. Chen ◽  
C. F. Chang ◽  
H. L. Tsay ◽  
H. D. Yang ◽  
J.-Y. Lin
Keyword(s):  
Magnetic Field ◽  
Low Temperature ◽  
Specific Heat ◽  
Field Dependence ◽  
Magnetic Field Dependence ◽  
Low Temperature Specific Heat
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