Gain, noise and intermodulation in a nonlinear superconducting resonator

A superconducting microwave resonator is modified with several weak links to make it nonlinear and operated as a phase-insensitive microwave amplifier. Signal gain is demonstrated by intermodulation with a strong pump. The gain is sharply frequency dependent, and we demonstrate phase dependence by e...

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Published in:EPJ quantum technology Vol. 1; no. 1; p. 1
Main Authors: Tholén, Erik A, Ergül, Adem, Schaeffer, David, Haviland, David B
Format: Journal Article
Language:English
Published: Berlin/Heidelberg Springer Berlin Heidelberg 01-12-2014
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Abstract A superconducting microwave resonator is modified with several weak links to make it nonlinear and operated as a phase-insensitive microwave amplifier. Signal gain is demonstrated by intermodulation with a strong pump. The gain is sharply frequency dependent, and we demonstrate phase dependence by examining correlations between the signal and one idler which is a 3rd order intermodulation product of the pump and signal tones. A calibration procedure is described which is based on measurement of both thermal and quantum noise, revealing that the following HEMT amplifier adds noise at 15 times the quantum limit. When operated as a phase-insensitive amplifier the nonlinear resonator added noise at 2.5 times the quantum limit. Significant power is found at intermodulation products beyond 3rd order, which may be responsible for the inability to reach the quantum limit. PACS Codes: 74.78.-w, 42.65.Yj, 85.25.Cp.
AbstractList A superconducting microwave resonator is modified with several weak links to make it nonlinear and operated as a phase-insensitive microwave amplifier. Signal gain is demonstrated by intermodulation with a strong pump. The gain is sharply frequency dependent, and we demonstrate phase dependence by examining correlations between the signal and one idler which is a 3rd order intermodulation product of the pump and signal tones. A calibration procedure is described which is based on measurement of both thermal and quantum noise, revealing that the following HEMT amplifier adds noise at 15 times the quantum limit. When operated as a phase-insensitive amplifier the nonlinear resonator added noise at 2.5 times the quantum limit. Significant power is found at intermodulation products beyond 3rd order, which may be responsible for the inability to reach the quantum limit
A superconducting microwave resonator is modified with several weak links to make it nonlinear and operated as a phase-insensitive microwave amplifier. Signal gain is demonstrated by intermodulation with a strong pump. The gain is sharply frequency dependent, and we demonstrate phase dependence by examining correlations between the signal and one idler which is a 3rd order intermodulation product of the pump and signal tones. A calibration procedure is described which is based on measurement of both thermal and quantum noise, revealing that the following HEMT amplifier adds noise at 15 times the quantum limit. When operated as a phase-insensitive amplifier the nonlinear resonator added noise at 2.5 times the quantum limit. Significant power is found at intermodulation products beyond 3rd order, which may be responsible for the inability to reach the quantum limit. PACS Codes: 74.78.-w, 42.65.Yj, 85.25.Cp.
A superconducting microwave resonator is modified with several weak links to make it nonlinear and operated as a phase-insensitive microwave amplifier. Signal gain is demonstrated by intermodulation with a strong pump. The gain is sharply frequency dependent, and we demonstrate phase dependence by examining correlations between the signal and one idler which is a 3rd order intermodulation product of the pump and signal tones. A calibration procedure is described which is based on measurement of both thermal and quantum noise, revealing that the following HEMT amplifier adds noise at 15 times the quantum limit. When operated as a phase-insensitive amplifier the nonlinear resonator added noise at 2.5 times the quantum limit. Significant power is found at intermodulation products beyond 3rd order, which may be responsible for the inability to reach the quantum limit. PACS Codes: 74.78.-w, 42.65.Yj, 85.25.Cp.
ArticleNumber 5
Author Ergül, Adem
Tholén, Erik A
Haviland, David B
Schaeffer, David
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Cites_doi 10.1103/PhysRevLett.7.118
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10.1038/nphys1090
10.1038/nature06126
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10.1038/nature09035
ContentType Journal Article
Copyright Tholén et al.; licensee Springer on behalf of EPJ. 2014. This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License ( ), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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Keywords intermodulation
quantum noise
parametric amplifier
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Snippet A superconducting microwave resonator is modified with several weak links to make it nonlinear and operated as a phase-insensitive microwave amplifier. Signal...
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SubjectTerms 3rd order intermodulation products
Calibration procedure
Frequency dependent
Inter-modulation products
Intermodulation
Microwave amplifiers
Microwave Quantum Optics
Microwave resonators
Nanotechnology and Microengineering
Nonlinear resonators
Parametric amplifiers
Phase dependence
Phase-insensitive amplifiers
Physics
Physics and Astronomy
Quantum Information Technology
Quantum noise
Quantum Physics
Spintronics
Superconducting microwave resonators
Superconducting resonators
Title Gain, noise and intermodulation in a nonlinear superconducting resonator
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