The specific heat capacity of a substance is a very useful thermodynamic quantitiy.
All internal degrees of freedom contribute to it and can be determined as a function of magnetic field and temperature.
Especially superconducting and magnetic phase transitions show up as anomalies in the specific heat capacity.
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The figure shows two silver sample holders to which the sample, a heater, and a thermometer are thermally
coupled by thin wires of well defined thermal conductivity. The device can be screwed to the cold finger
of a dilution refrigerator and be cooled to about 10 mK. Visible are also the electrical leads to the
thermometers and heaters.
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The main method for measuring the specific heat capacity is the so called semiadiabatic heat pulse technique.
The sample along with a tiny heater and a small thermometer is connected to the sample holder by a "weak thermal link".
The platform is cooled to a final temperature Tbase given by the temperature of the cold finger,
the thermal conductance of the weak link and the residual heat leak.
When a well defined heat puls ΔQ is applied, the sample along with the so called addendum (heater and thermometer)
is heated to a slightly higher temperature Tbase + ΔT and relaxes back to Tbase with a time constant
τ = Rthermal · C.
The specific heat capacity at Tbase + ½ΔT is given by c = ΔQ/ΔT.
The procedure is repeated at various temperatures Tbase and the specific heat capacity is thus determined as a function of T.