Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physical Review

Quantum Theory of a Damped Electrical Oscillator and Noise. II. The Radiation Resistance

J WEBER

Published Sep 15, 1954• 1 citation
Publisher
DOI
10.1103/physrev.95.1706

Related papers

Quantum Theory of Damped Oscillation II

Shigemi Araki

酪農学園大学紀要. 自然科学編•Oct 1, 1985•0 citations

Quantum Theory of Damped Oscillation II

Shigemi Araki

•Oct 1, 1985•0 citations

Internal and external field fluctuations of a laser oscillator: Part II--Electrical circuit theory

OLLE NILSSON, Y. Yamamoto, S. Machida

The amplitude and phase noise spectra of the internal and external fields of a negative resistance oscillator are derived using electrical circuit theory. It is shown that the difference between internal and external fluctuations becomes important in the quantum domain (h\omega > kT) where external noise sources are not negligible as they often are in the classical domain (h\omega < kT). Using established methods to describe quantum fluctuations in electrical circuits, we obtain results in full agreement with the more exact but less general direct quantum mechanical analysis of a Fabry-Perot laser in Part I.

IEEE Journal of Quantum Electronics•Oct 1, 1986•28 citations

Quantum theory of the damped harmonic oscillator

Hermann Grabert, Ulrich Weiß, Peter Talkner A

The European Physical Journal B•Mar 1, 1984•272 citations

Radiation and noise in quantum electronics

William H. Louisell

•Jan 1, 1964•342 citations

Noise characteristics of a dc SQUID with a resistively shunted inductance. II. Optimum damping

Keiji Enpuku, Keiji Yoshida, Satoshi Kohjiro

Effects of a damping resistance on noise characteristics of a dc SQUID are studied theoretically, where the damping resistance is in shunt with a loop inductance of the SQUID. An analytical expression for the energy resolution of the SQUID is obtained, with which the relation between the damping resistance and the energy resolution is studied in detail. It is shown that an optimum value of the damping resistance exists, which is determined by the tradeoff between the improvement of the transfer function and the additional noise due to the damping resistance. Optimum values of the damping resistance are about twice the shunt resistance of the SQUID and vary slightly with SQUID modulation parameter β. For optimum damping, the energy resolution is improved, compared with the case without the damping resistance. This means that the SQUID with large β can be used without significant degradation of the performance, i.e., the previous restriction of β=1 can be loosened. The analytical results agree quantitatively with numerical ones.

Journal of Applied Physics•Dec 15, 1986•66 citations
The amplitude and phase noise spectra of the internal and external fields of a negative resistance oscillator are derived using electrical circuit theory. It is shown that the difference between internal and external fluctuations becomes important in the quantum domain (h\omega > kT) where external noise sources are not negligible as they often are in the classical domain (h\omega < kT). Using established methods to describe quantum fluctuations in electrical circuits, we obtain results in full agreement with the more exact but less general direct quantum mechanical analysis of a Fabry-Perot laser in Part I.
Effects of a damping resistance on noise characteristics of a dc SQUID are studied theoretically, where the damping resistance is in shunt with a loop inductance of the SQUID. An analytical expression for the energy resolution of the SQUID is obtained, with which the relation between the damping resistance and the energy resolution is studied in detail. It is shown that an optimum value of the damping resistance exists, which is determined by the tradeoff between the improvement of the transfer function and the additional noise due to the damping resistance. Optimum values of the damping resistance are about twice the shunt resistance of the SQUID and vary slightly with SQUID modulation parameter β. For optimum damping, the energy resolution is improved, compared with the case without the damping resistance. This means that the SQUID with large β can be used without significant degradation of the performance, i.e., the previous restriction of β=1 can be loosened. The analytical results agree quantitatively with numerical ones.