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 Applied

Squeezing of light in a dual-pumped microresonator revealed by a common-pass local oscillator

A. N. Danilin, Timur R. Yunusov, Alexey P. Dushanin, Natalia S. Salakhova, Alexander K. Vorobyev, Alexey D. Ivanov, Anatoly Viktorovich Masalov, Igor A. Bilenko, Dmitry A. Chermoshentsev

Published Apr 10, 2026• 0 citations
Publisher
DOI
10.1103/f5dv-12fk

Related papers

Experimental Study of Squeezed States Generation Optimal Regimes in Dual-pumped On-chip Microresonators

Alexander K. Vorobyev, Nikolay A. Kapridov, Georgii V. Grechko +4 more

We perform an experimental optimization of squeezed light generation via degenerate optical parametric oscillation process in dual-pumped integrated microresonators. This process is sensitive to the power and frequency detunings of the pumps, and the threshold of this process depends on the spectral interval between pumps.

Quantum 2.0 Conference and Exhibition•Jan 1, 2023•0 citations

Squeezing by second-harmonic generation in a monolithic resonator

P. K�rz, R. Paschotta, K. Fiedler +3 more

Applied Physics B•Sep 1, 1992•40 citations

Squeezing states of light in a surface nanoscale axial photonics microresonator

Anonymous

Physical Review A•Sep 11, 2026•0 citations

Single-beam squeezing in a Doppler broadened medium

Seng‐Tiong Ho, N. C. Wong, Jeffrey H. Shapiro +1 more

We have generated squeezed states of light with a single pump beam propagating through Doppler broadened sodium vapor via forward four-wave mixing (FWM) with spatially degenerate pump and probe modes. The two probe-mode inputs are vacuum states at nondegenerate frequencies, which are transformed to squeezed vacuum by the FWM interaction. Compared with previous FWM configurations,1 this single-pass single-pump-beam configuration ensures maximal overlap of the four interacting beams, thus maximizing the squeezing nonlinearity and improving the overall efficiency. The transmitted pump has the wrong phase to act as the local oscillator for detecting the squeezed spectrum.1 Therefore, a cavity is used to filter out most of the transmitted pump intensity, and the squeezed vacuum is detected with another local oscillator using the standard dual-detector scheme. The residual pump beam provides a reference to monitor the phase between the pump and squeezed vacuum. The observed 0.8-dB reduction in the shot noise corresponds to an inferred 50% squeezing of the light at the exit of the vapor medium, which is in reasonable agreement with the theory given by Ho et al. 2 A linearly polarized pump is found to give less squeezing than a circularly polarized pump, possibly due to optical pumping.

Annual Meeting Optical Society of America•Jan 1, 1988•0 citations

Phase locking scheme for squeezed vacuum generated by single-pass optical parametric amplifier

Yoshitaka Taguchi, Yasuyuki Ozeki

Single-pass optical parametric amplification (OPA) is attractive in the generation of broadband squeezed vacuum. To achieve a higher squeezing level, precise control of the local oscillator (LO) phase is needed. However, the conventional control scheme was designed for squeezing by optical parametric oscillation (OPO). In this study, we propose a new scheme, which is applicable to single-pass OPA. In this scheme, we measure the modulation in the residual pump light after the OPA crystal to realize precise phase-locking of the LO. We anticipate that the proposed scheme will be indispensable for practical applications of squeezing with single-pass OPA.

Optical and Quantum Sensing and Precision Metrology II•Mar 3, 2022•0 citations

Squeezed light from a single emitter coupled to a nanostructure

Diego Martín-Cano, Harald R. Haakh, Murr K +1 more

•Jan 1, 2014•0 citations
We have generated squeezed states of light with a single pump beam propagating through Doppler broadened sodium vapor via forward four-wave mixing (FWM) with spatially degenerate pump and probe modes. The two probe-mode inputs are vacuum states at nondegenerate frequencies, which are transformed to squeezed vacuum by the FWM interaction. Compared with previous FWM configurations,1 this single-pass single-pump-beam configuration ensures maximal overlap of the four interacting beams, thus maximizing the squeezing nonlinearity and improving the overall efficiency. The transmitted pump has the wrong phase to act as the local oscillator for detecting the squeezed spectrum.1 Therefore, a cavity is used to filter out most of the transmitted pump intensity, and the squeezed vacuum is detected with another local oscillator using the standard dual-detector scheme. The residual pump beam provides a reference to monitor the phase between the pump and squeezed vacuum. The observed 0.8-dB reduction in the shot noise corresponds to an inferred 50% squeezing of the light at the exit of the vapor medium, which is in reasonable agreement with the theory given by Ho et al. 2 A linearly polarized pump is found to give less squeezing than a circularly polarized pump, possibly due to optical pumping.
Single-pass optical parametric amplification (OPA) is attractive in the generation of broadband squeezed vacuum. To achieve a higher squeezing level, precise control of the local oscillator (LO) phase is needed. However, the conventional control scheme was designed for squeezing by optical parametric oscillation (OPO). In this study, we propose a new scheme, which is applicable to single-pass OPA. In this scheme, we measure the modulation in the residual pump light after the OPA crystal to realize precise phase-locking of the LO. We anticipate that the proposed scheme will be indispensable for practical applications of squeezing with single-pass OPA.