Low-temperature specific heat and thermal conductivity of a glassy polymer under applied pressure

1989 ◽  
Vol 40 (3) ◽  
pp. 1901-1917 ◽  
Author(s):  
J. M. Grace ◽  
A. C. Anderson
Keyword(s):  
Thermal Conductivity ◽  
Low Temperature ◽  
Specific Heat ◽  
Glassy Polymer ◽  
Applied Pressure ◽  
Low Temperature Specific Heat

Low temperature specific heat and thermal conductivity of antiferromagnetic Kondo alloy CePdGa

1996 ◽  
Vol 46 (S5) ◽  
pp. 2589-2590 ◽  
Author(s):  
S. Chastin ◽  
D. T. Adroja ◽  
D. F. Brewer ◽  
T. Hargreaves ◽  
C. S. McMenamin ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
Low Temperature ◽  
Specific Heat ◽  
Low Temperature Specific Heat

Low-temperature specific heat and thermal conductivity of glasses

1993 ◽  
Vol 70 (2) ◽  
pp. 182-185 ◽  
Author(s):  
L. Gil ◽  
M. A. Ramos ◽  
A. Bringer ◽  
U. Buchenau
Keyword(s):  
Thermal Conductivity ◽  
Low Temperature ◽  
Specific Heat ◽  
Low Temperature Specific Heat

Low-temperature specific heat and thermal conductivity of silica aerogels

1992 ◽  
Vol 145 ◽  
pp. 202-206 ◽  
Author(s):  
A. Bernasconi ◽  
T. Sleator ◽  
D. Posselt ◽  
J.K. Kjems ◽  
H.R. Ott
Keyword(s):  
Thermal Conductivity ◽  
Low Temperature ◽  
Specific Heat ◽  
Silica Aerogels ◽  
Low Temperature Specific Heat

LOW-TEMPERATURE SPECIFIC HEAT OF YMn2 IN THE PARAMAGNETIC AND ANTIFERROMAGNETIC PHASES

1993 ◽  
Vol 07 (01n03) ◽  
pp. 830-833 ◽  
Author(s):  
R.A. FISHER ◽  
R. BALLOU ◽  
J.P. EMERSON ◽  
E. LELIEVRE-BERNA ◽  
N.E. PHILLIPS
Keyword(s):  
Low Temperature ◽  
Specific Heat ◽  
Applied Pressure ◽  
Paramagnetic State ◽  
Linear Term ◽  
Spin Fluctuations ◽  
Spin Frustration ◽  
Magnetic Instability ◽  
Low Temperature Specific Heat

The low-temperature specific heat of YMn2 has been measured at applied pressures of 0 to 7.7 kbar. A paramagnetic state is stabilized for moderate values of the applied pressure (of the order of 1.6 kbar). A large linear term in the specific heat, which decreases regularly with increasing pressure, is observed in this phase. It is ascribed to giant spin fluctuations associated with a magnetic-non magnetic instability and a strong geometrical spin frustration.

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