Markovian Dynamics of Josephson Parametric Amplification
In this work, we derive the dynamics of the lossy DC pumped non-degenerate Josephson parametric amplifier (DCPJPA). The main element in a DCPJPA is the superconducting Josephson junction. The DC bias generates the AC Josephson current varying the nonlinear inductance of the junction. By this way...
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2017-09-01
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doaj-c56274731bfb4afabf6085773e2105c92020-11-24T22:10:10ZdeuCopernicus PublicationsAdvances in Radio Science 1684-99651684-99732017-09-011513114010.5194/ars-15-131-2017Markovian Dynamics of Josephson Parametric AmplificationW. Kaiser0M. Haider1J. A. Russer2P. Russer3C. Jirauschek4Institute for Nanoelectronics, Technical University of Munich, Arcisstraße 21, 80333 Munich, GermanyInstitute for Nanoelectronics, Technical University of Munich, Arcisstraße 21, 80333 Munich, GermanyInstitute for Nanoelectronics, Technical University of Munich, Arcisstraße 21, 80333 Munich, GermanyInstitute for Nanoelectronics, Technical University of Munich, Arcisstraße 21, 80333 Munich, GermanyInstitute for Nanoelectronics, Technical University of Munich, Arcisstraße 21, 80333 Munich, GermanyIn this work, we derive the dynamics of the lossy DC pumped non-degenerate Josephson parametric amplifier (DCPJPA). The main element in a DCPJPA is the superconducting Josephson junction. The DC bias generates the AC Josephson current varying the nonlinear inductance of the junction. By this way the Josephson junction acts as the pump oscillator as well as the time varying reactance of the parametric amplifier. In quantum-limited amplification, losses and noise have an increased impact on the characteristics of an amplifier. We outline the classical model of the lossy DCPJPA and derive the available noise power spectral densities. A classical treatment is not capable of including properties like spontaneous emission which is mandatory in case of amplification at the quantum limit. Thus, we derive a quantum mechanical model of the lossy DCPJPA. Thermal losses are modeled by the quantum Langevin approach, by coupling the quantized system to a photon heat bath in thermodynamic equilibrium. The mode occupation in the bath follows the Bose-Einstein statistics. Based on the second quantization formalism, we derive the Heisenberg equations of motion of both resonator modes. We assume the dynamics of the system to follow the Markovian approximation, i.e. the system only depends on its actual state and is memory-free. We explicitly compute the time evolution of the contributions to the signal mode energy and give numeric examples based on different damping and coupling constants. Our analytic results show, that this model is capable of including thermal noise into the description of the DC pumped non-degenerate Josephson parametric amplifier.https://www.adv-radio-sci.net/15/131/2017/ars-15-131-2017.pdf |
collection |
DOAJ |
language |
deu |
format |
Article |
sources |
DOAJ |
author |
W. Kaiser M. Haider J. A. Russer P. Russer C. Jirauschek |
spellingShingle |
W. Kaiser M. Haider J. A. Russer P. Russer C. Jirauschek Markovian Dynamics of Josephson Parametric Amplification Advances in Radio Science |
author_facet |
W. Kaiser M. Haider J. A. Russer P. Russer C. Jirauschek |
author_sort |
W. Kaiser |
title |
Markovian Dynamics of Josephson Parametric Amplification |
title_short |
Markovian Dynamics of Josephson Parametric Amplification |
title_full |
Markovian Dynamics of Josephson Parametric Amplification |
title_fullStr |
Markovian Dynamics of Josephson Parametric Amplification |
title_full_unstemmed |
Markovian Dynamics of Josephson Parametric Amplification |
title_sort |
markovian dynamics of josephson parametric amplification |
publisher |
Copernicus Publications |
series |
Advances in Radio Science |
issn |
1684-9965 1684-9973 |
publishDate |
2017-09-01 |
description |
In this work, we derive the dynamics of the lossy DC pumped non-degenerate
Josephson parametric amplifier (DCPJPA). The main element in a DCPJPA is the
superconducting Josephson junction. The DC bias generates the AC Josephson
current varying the nonlinear inductance of the junction. By this way the
Josephson junction acts as the pump oscillator as well as the time varying
reactance of the parametric amplifier. In quantum-limited amplification,
losses and noise have an increased impact on the characteristics of an
amplifier. We outline the classical model of the lossy DCPJPA and derive the
available noise power spectral densities. A classical treatment is not
capable of including properties like spontaneous emission which is mandatory
in case of amplification at the quantum limit. Thus, we derive a quantum
mechanical model of the lossy DCPJPA. Thermal losses are modeled by the
quantum Langevin approach, by coupling the quantized system to a photon heat
bath in thermodynamic equilibrium. The mode occupation in the bath follows
the Bose-Einstein statistics. Based on the second quantization formalism, we
derive the Heisenberg equations of motion of both resonator modes. We assume
the dynamics of the system to follow the Markovian approximation, i.e. the
system only depends on its actual state and is memory-free. We explicitly
compute the time evolution of the contributions to the signal mode energy and
give numeric examples based on different damping and coupling constants. Our
analytic results show, that this model is capable of including thermal noise
into the description of the DC pumped non-degenerate Josephson parametric
amplifier. |
url |
https://www.adv-radio-sci.net/15/131/2017/ars-15-131-2017.pdf |
work_keys_str_mv |
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