2020
DOI: 10.1103/physrevb.102.214514
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Electron cooling by phonons in superconducting proximity structures

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Cited by 9 publications
(7 citation statements)
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“…Since is related to the overheating phenomena and to the heat exchange, its amplitude and the temperature at which it appears should depend on the length of the junction, its environment as well as on microscopic mechanisms in play. For instance, the efficiency of the heat exchange via electron-phonon mechanism has strong temperature dependence in the dirty limit 29 ( Supplementary Materials ) and provides good thermal equilibrium between electron and phonon baths at temperatures above 1K 1 , 2 , 30 , 31 . Our experimental conditions are close to the case when the exchange between the electron and phonon baths is proportional to , where U is the volume of the NW 29 .…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Since is related to the overheating phenomena and to the heat exchange, its amplitude and the temperature at which it appears should depend on the length of the junction, its environment as well as on microscopic mechanisms in play. For instance, the efficiency of the heat exchange via electron-phonon mechanism has strong temperature dependence in the dirty limit 29 ( Supplementary Materials ) and provides good thermal equilibrium between electron and phonon baths at temperatures above 1K 1 , 2 , 30 , 31 . Our experimental conditions are close to the case when the exchange between the electron and phonon baths is proportional to , where U is the volume of the NW 29 .…”
Section: Resultsmentioning
confidence: 99%
“…For instance, the efficiency of the heat exchange via electron-phonon mechanism has strong temperature dependence in the dirty limit 29 ( Supplementary Materials ) and provides good thermal equilibrium between electron and phonon baths at temperatures above 1K 1 , 2 , 30 , 31 . Our experimental conditions are close to the case when the exchange between the electron and phonon baths is proportional to , where U is the volume of the NW 29 . Other channels of the heat removal from the system are significantly limited, due to a poor link of the NW to substrate and to superconducting electrodes.…”
Section: Resultsmentioning
confidence: 99%
“…The second channel is the transfer of excess energy to phonons. In dirty metals, the rate of this process , P e-ph , is given by [77] P e-ph = K * 3ζ(5) 3π…”
Section: A Dissipated and Absorbed Powermentioning
confidence: 99%
“…The nanofabricated detector of worked in the regime where the measurement cut-off frequency was 10 kHz, which falls somewhat below 1/τ . Furthermore the metallic absorber was proximitized by a superconducting contact further decreasing C and G th (Heikkilä and Giazotto, 2009;Nikolic et al, 2020) and this way improving its performance. The experiment (Fig.…”
Section: E Energy Sensitivity Of a Calorimetermentioning
confidence: 99%