High-sensitivity tool for studying phonon related mechanical losses in low loss materials

GND
1023589036
Zugehörigkeit
Institute of Solid State Physics, Friedrich-Schiller-University Jena, Helmholtzweg 5, D-07743 Jena, Germany
Heinert, D.;
GND
134123662
Zugehörigkeit
Institute of Solid State Physics, Friedrich-Schiller-University Jena, Helmholtzweg 5, D-07743 Jena, Germany
Zimmer, A.;
GND
134276663
Zugehörigkeit
Institute of Solid State Physics, Friedrich-Schiller-University Jena, Helmholtzweg 5, D-07743 Jena, Germany
Nawrodt, R.;
GND
134156161
Zugehörigkeit
Institute of Solid State Physics, Friedrich-Schiller-University Jena, Helmholtzweg 5, D-07743 Jena, Germany
Koettig, T.;
GND
102778531X
Zugehörigkeit
Institute of Solid State Physics, Friedrich-Schiller-University Jena, Helmholtzweg 5, D-07743 Jena, Germany
Schwarz, C.;
GND
1328250636
Zugehörigkeit
Institute of Solid State Physics, Friedrich-Schiller-University Jena, Helmholtzweg 5, D-07743 Jena, Germany
Hudl, M.;
GND
132825206X
Zugehörigkeit
Institute of Solid State Physics, Friedrich-Schiller-University Jena, Helmholtzweg 5, D-07743 Jena, Germany
Vodel, W.;
GND
113119321
Zugehörigkeit
Institute of Applied Physics, Friedrich-Schiller-University Jena, Max-Wien-Platz 1, D-07743 Jena, Germany
Tünnermann, A.;
GND
1068849649
Zugehörigkeit
Institute of Solid State Physics, Friedrich-Schiller-University Jena, Helmholtzweg 5, D-07743 Jena, Germany
Seidel, P.

Fundamental mechanical loss mechanisms exist even in very pure materials, for instance, due to the interactions of excited acoustic waves with thermal phonons. A reduction of these losses in a certain frequency range is desired in high precision instruments like gravitational wave detectors. Systematic analyses of the mechanical losses in those low loss materials are essential for this aim, performed in a highly sensitive experimental set-up. Our novel method of mechanical spectroscopy, cryogenic resonant acoustic spectroscopy of bulk materials (CRA spectroscopy), is well suited to systematically determine losses at the resonant frequencies of the samples of less than 10 -9 in the wide temperature range from 5 to 300 K. A high precision set-up in a specially built cryostat allows contactless excitation and readout of the oscillations of the sample. The experimental set-up and measuring procedure are described. Limitations to our experiment due to external loss mechanisms are analysed. The influence of the suspension system as well as the sample preparation is explained.

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