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Ph.D. thesis (pdf) - dirac

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5.1. Dielectric spectroscopy 73<br />

with a thickness of 0.5 mm in order to ensure that the pressure is well transmitted<br />

from the compression liquid to the sample liquid.<br />

Figure 5.1: The experimental setup for dielectric spectroscopy under pressure at<br />

Orsay. The Teflon parts shown in grey to distinguish from the metal. The length<br />

of the autoclave is ∼ 30 cm, the Teflon cell is 5 cm long. The parts are shown<br />

separately in appendix C.<br />

The advantage of this setup, compared to other setups for dielectric spectroscopy<br />

under pressure, is that it ensures a hydrostatic pressure because the sample is compressed<br />

from all sides. It is moreover possible to take spectra both under compression<br />

and decompression, and it can hence be verified that there is no hysteresis in the<br />

system.<br />

The capacitor used for the measurement is composed by two gold coated electrodes<br />

separated by small Teflon spacers. The distance between the capacitor plates is<br />

adjustable and the area is 5.44 cm 2 . We report data measured with a plate distance<br />

of 0.3 mm giving an empty capacitance of 16 pF. The strength of the measured<br />

signal is proportional to the area and inversely proportional to the distance between<br />

the plates. It is therefore an advantage, especially for measurements on systems<br />

with small dipole moments, to maximize the area and minimize the plate distance.<br />

Although the area is limited by the dimensions of the pressure cell, the distance<br />

could in principle be smaller; however it is crucial that the plates do not touch, even<br />

when the pressure is applied, as this would lead to an electrical short cut.

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