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

Optics Communications

Nonlinear amplification in a second-harmonic-generating system

P. L. Chu, Boris A. Malomed, Gang‐Ding Peng

Published Jul 1, 1996• 9 citations
Publisher
DOI
10.1016/0030-4018(96)00132-0

Related papers

Effect of pump fluctuations on second harmonic generation and parametric amplifications

NILOY KUMAR DUTTA

Optical and Quantum Electronics•May 1, 1979•14 citations

Processes of second harmonic generation and degenerate parametric amplification in a selectively absorbing medium

В. Г. Андреев, О. А. Васильева, Evgueny A. Lapshin +1 more

•Jan 1, 1985•0 citations

Nonlinear quantum effects in second-harmonic generation

Daniel F. Walls, C. T. Tindle

Lettere al nuovo cimento della societa italiana di fisica/Lettere al nuovo cimento•Oct 1, 1971•25 citations

Broadband optical parametric amplification using PPLN waveguide pumped by detuned second harmonic

Masaki Asobe, Daiki Yagi, Yuki Kawabata +4 more

Optical parametric amplification in the range of 1.3–1.8 µm was demonstrated by using a periodically poled LiNbO3 (PPLN) waveguide as a nonlinear medium by varying the detuning of the pump wavelength. A wide range of detuning was enabled by using a multiple-quasi-phase-matched (M-QPM) LiNbO3 waveguide for pump generation through second harmonic generation (SHG) and temperature control of the PPLN waveguide. Broadband optical amplification and wavelength conversion through difference frequency generation (DFG) are considered useful for widening the bandwidth of optical communication.

Optics Express•Mar 2, 2022•11 citations

Existence of a threshold for second-harmonic generation inside high-confinement microresonators as a consequence of the generalized creation and annihilation operators

Marc Collette, Serge Gauvin

This work presents a quantum theory of the nonlinear optical process of second-harmonic generation (SHG) in one-dimensional microresonators. More specifically, we show how the manipulation of vacuum field fluctuations in high-confinement systems, leading to a spectrally (and spatially) modulated commutation relation for the photon's generalized formulations of their creation and annihilation operators, deeply affects SHG behavior and gives rise to a threshold level. The two main effects the modulated commutator has on this optical process are an inhibition of the SHG process at low pumping level and a significant (cubic) amplification of the second-harmonic signal production rate once the threshold is overcome (finally reaching the usual quadratic dependence at sufficiently high pumping level). Our predictions, which represent a concrete picture of a fractional quantum system, could be used to probe vacuum field fluctuations present in high-confinement microresonators and emphasize the fundamental importance of vacuum field fluctuations.

Physical Review A•Jul 29, 2022•1 citation

Transient regime in second harmonic generation

Jacob Szeftel, Laure Sandeau, Nicolas Sandeau +2 more

Optics Communications•May 13, 2013•2 citations
Optical parametric amplification in the range of 1.3–1.8 µm was demonstrated by using a periodically poled LiNbO3 (PPLN) waveguide as a nonlinear medium by varying the detuning of the pump wavelength. A wide range of detuning was enabled by using a multiple-quasi-phase-matched (M-QPM) LiNbO3 waveguide for pump generation through second harmonic generation (SHG) and temperature control of the PPLN waveguide. Broadband optical amplification and wavelength conversion through difference frequency generation (DFG) are considered useful for widening the bandwidth of optical communication.
This work presents a quantum theory of the nonlinear optical process of second-harmonic generation (SHG) in one-dimensional microresonators. More specifically, we show how the manipulation of vacuum field fluctuations in high-confinement systems, leading to a spectrally (and spatially) modulated commutation relation for the photon's generalized formulations of their creation and annihilation operators, deeply affects SHG behavior and gives rise to a threshold level. The two main effects the modulated commutator has on this optical process are an inhibition of the SHG process at low pumping level and a significant (cubic) amplification of the second-harmonic signal production rate once the threshold is overcome (finally reaching the usual quadratic dependence at sufficiently high pumping level). Our predictions, which represent a concrete picture of a fractional quantum system, could be used to probe vacuum field fluctuations present in high-confinement microresonators and emphasize the fundamental importance of vacuum field fluctuations.