Electron-phonon coupling in layered nanostructures at low temperatures
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2020-10-13 11:06
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COJOCARU, Sergiu. Electron-phonon coupling in layered nanostructures at low temperatures. In: Materials Science and Condensed Matter Physics, Ed. 8-th Edition, 12-16 septembrie 2016, Chişinău. Chişinău: Institutul de Fizică Aplicată, 2016, Editia 8, p. 46. ISBN 978-9975-9787-1-2.
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Materials Science and Condensed Matter Physics
Editia 8, 2016
Conferința "International Conference on Materials Science and Condensed Matter Physics"
8-th Edition, Chişinău, Moldova, 12-16 septembrie 2016

Electron-phonon coupling in layered nanostructures at low temperatures


Pag. 46-46

Cojocaru Sergiu
 
Horia Hulubei National Institute for Physics and Nuclear Engineering
 
 
Disponibil în IBN: 18 iulie 2019


Rezumat

Electron-phonon coupling is studied for acoustically non-uniform layered nanostructures consisting of a metal film deposited on an insulating membrane. Electrons are heated by an external source to a temperature higher than the temperature of the crystal lattice ( Te > Tp ) and the resulting heat flux transferred from electrons to phonons is considered for a low temperature regime. The system is representative of the central element in the electronic microrefrigerators designed for the on-chip cooling of ultrasensitive detectors far down to the sub-Kelvin region [1]. For the total thickness below 100-200 nm the phonon subsytem is dominated by long wavelength vibrations and can be treated in terms of an effectively quasi-two-dimensional elastic medium with a dramatic enhancement of the heat transfer over the bulk material [2,3]. By assuming the deformation potential mechanism of coupling, an explicit expression for the electron-phonon heat flux is derived analytically by taking into account the acoustic non-uniformity of the device.   The obtained results explain the behavior observed in some experiments including the case of Cu film supported by a SiN insulating membrane. It is shown that the main contribution to the heat flux is due to the electron coupling with Lamb’s dilatational and flexural acoustic modes in a roughly comparable amount. The role of the flexural modes increases as the thickness of the film decreases.