Engineering Physics of Superconducting Hot-Electron Bolometer Mixers

Journal Article (2017)
Author(s)

Teun Klapwijk (Kavli institute of nanoscience Delft, TU Delft - QN/Klapwijk Lab)

Alexander Semenov (Moscow State Pedagogical University)

Research Group
QN/Klapwijk Lab
Copyright
© 2017 T.M. Klapwijk, A. V. Semenov
DOI related publication
https://doi.org/10.1109/TTHZ.2017.2758267
More Info
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Publication Year
2017
Language
English
Copyright
© 2017 T.M. Klapwijk, A. V. Semenov
Research Group
QN/Klapwijk Lab
Issue number
6
Volume number
7
Pages (from-to)
627-648
Reuse Rights

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Abstract

Superconducting hot-electron bolometers are presently the best performing mixing devices for the frequency range beyond 1.2 THz, where good-quality superconductor-insulator-superconductor devices do not exist. Their physical appearance is very simple: an antenna consisting of a normal metal, sometimes a normal-metal-superconductor bilayer, connected to a thin film of a narrow short superconductor with a high resistivity in the normal state. The device is brought into an optimal operating regime by applying a dc current and a certain amount of local-oscillator power. Despite this technological simplicity, its operation has found to be controlled by many different aspects of superconductivity, all occurring simultaneously. A core ingredient is the understanding that there are two sources of resistance in a superconductor: a charge-conversion resistance occurring at a normal-metal-superconductor interface and a resistance due to time-dependent changes of the superconducting phase. The latter is responsible for the actual mixing process in a nonuniform superconducting environment set up by the bias conditions and the geometry. The present understanding indicates that further improvement needs to be found in the use of other materials with a faster energy relaxation rate. Meanwhile, several empirical parameters have become physically meaningful indicators of the devices, which will facilitate the technological developments.

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