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

Journal of the Optical Society of America B

All-optical frequency-controlled frequency switch

Taciano Amaral Sorrentino, Orlando Di Lorenzo, L. C. de Oliveira, Martine Chevrollier, Marcos Oriá

Published Jun 21, 2010• 7 citations
Publisher

Abstract

Orthogonally polarized optical feedback has been proven to act on the frequency of semiconductor lasers. The coupling of this feedback to a nonlinear filter results in bistability for the frequency of the laser output [Phys. Rev. Lett.94, 173902 (2005)]. This phenomenon opens the way to the development of all-optical devices such as a switch between frequency states of the optical emission. For demonstrating this particular application we use an AsGaAl monomode laser emitting around 852 nm, together with a warm atomic cesium vapor as a resonant filter. The output frequency state of the switch is determined by two different frequencies of a control laser, with each control frequency changing the switch frequency in only one direction.

DOI
10.1364/josab.27.001458

Related papers

All-optical FM switch

Taciano Amaral Sorrentino, Martine Chevrollier, Marcos Oriá

We use the dynamic frequency response of a semiconductor laser submitted to an orthogonal-polarization feedback field to develop configurations of all-optical device such as a frequency converser, an amplitudefrequency converter and a switch between frequency states. Here we discuss particularly this last application. The laser used is a monomode 852 nm AsGaAl emitting around the D2 Cs line of a hot atomic vapor.

•Jan 1, 2006•0 citations

Dinâmica em freqüência de lasers semicondutores sobrealimentação ótica ortogonal e aplicação: chaveamentotodo-ótico em frequência

Taciano Amaral Sorrentino

We analyze the dynamics of semiconductor lasers radiation frequency when these lasers are subject to different conditions of optical feedback, and we demonstrate how it is possible to control the emission frequency using the different configurations explored. In the first system studied a semiconductor laser is fed back with light which polarization is orthogonal to the output polarization, spectrally filtered by a cesium atomic vapor. This system, besides presenting an effective technique to stabilize the laser frequency and reduce the laser linewidth, was the first to exhibit frequency bistable and multistable optical regimes with amplitude practically constant. This unique feature opens the way for applications in all-optical FM logical devices. The bistable and multistable regimes are interpreted through a phenomenological model, and, for the bistable regime, we discuss a rate equation model, built taking in account thermal effects and gain saturation. We also present an all-optical frequency switch, the first of his kind. The second system is used to investigate the behavior of the emission frequency of a semiconductor laser with an external cavity, inside which is placed an atomic filter. For different values of the injection current we observe the laser frequency locking in the atomic line, bistability and reproducible frequency instabilities.

•Jun 30, 2010•0 citations

Controllable frequency hysteresis in semiconductor lasers

Samuel B. Alves, Hugo L. D. de S. Cavalcante, Martine Chevrollier +2 more

Optical feedback with orthogonal polarization enables frequency sweep of semiconductor lasers and leads to frequency bistability when a resonant medium is used to filter the reinjected radiation. Here, we explore a configuration with two lasers coupled through mutual injection. Each laser injects and receives light with a polarization orthogonal to the plane of emission. Both injections are independently filtered by a resonant atomic vapor. We show that this more versatile version also exhibits bistable states, and that it is possible to reduce the laser frequency jitter as well as to invert its frequency hysteresis cycle on demand (from counterclockwise to clockwise and vice versa). Experimental demonstration is done with diode lasers emitting around 780 nm, using Rb thermal vapors as nonlinear filters.

Journal of the Optical Society of America B•Feb 9, 2016•1 citation

Control of chirality of frequency hysteresis

Samuel B. Alves, Hugo L. D. de S. Cavalcante, Martine Chevrollier +2 more

Coupling two lasers through mutual orthogonal optical injection we observe frequency bistability when the injections are spectrally filtered. The hysteresis chirality may be changed on demand. We use diode lasers and rubidium vapors as filters.

Latin America Optics and Photonics Conference•Jan 1, 2016•0 citations

Frequency domain bistability of tunable laser with frequency-dependent feedback

Lixue Chen

Traditional frequency domain optical bistability(FDOB) devices with hybrid electro-optical feedback have low response speed and high noise fluctuations.Hence,a novel tunable laser FDOB device with an all-optical feedback was developed using a nonlinear fiber ring resonator as the frequency feedback element.Parametric equations of optical bistability were established according to the system's response to nonlinear process and frequency-dependent feedback.Based on the parametric equations,the characteristics and controllable operations of FDOB were analyzed.The switching response speed of the optical bistability was discussed.The analysis showed that the proposed all-fiber laser bistability device can effectively achieve intensity-driven and gain-driven optical bistability.The position and shape of the bistability hysteresis curve vary with the adjustment of gain or loss in the fiber ring resonator,hence realizing the controlled all-optical bistability operations.Sudden jumping of optical bistability in the frequency domain can be applied to monitor laser wavelength shift and achieve sensoring.The optical bistability response time is in the nanosecond order of magnitude and bistability switching is ultrafast.

Harbin Gongcheng Daxue Xuebao/Journal of Harbin Engineering University•Jan 1, 2008•0 citations

Polarization control mechanisms in vectorial bistable lasers for one-frequency systems

Guy Ropars, A. Le Floch, Roger Le Naour

The basic mechanisms of the polarization switching in vectorial bistable lasers are studied both theoretically and experimentally versus internal parameters. In particular, by scanning the frequency of a gas laser with two linearly polarized eigenstates, two quite different flipping processes with hysteresis occur according to the linear-phase-anisotropy value of the cavity. Indeed, when the anisotropy increases, rotation and inhibition mechanisms appear successively. The variations of the hysteresis loop for different anisotropy and excitation values are theoretically found to be opposed in the two processes. Additional evolutions of the polarization, such as multiple switchings in the inhibition mechanism and ``hybrid'' hysteresis loops, are predicted. The experiments, essentially performed on a monomode 3.39-\ensuremath{\mu}m $^{3}\mathrm{\ensuremath{-}}^{20}$Ne laser containing an adjustable linear phase anisotropy, confirm the existence of the two processes and their corresponding properties. These processes may also occur in other quasi-isotropic lasers versus other internal parameters, such as, for instance, the injection current in semiconductor lasers. In this case the TE and TM modes flip only in the inhibition mechanism when the bistability conditions are satisfied. The knowledge of the basic flipping mechanisms in the laser itself enables us to understand and realize the external optical-polarization control by an anisotropic feedback (one-frequency systems). Induced-rotation and induced-inhibition mechanisms are then theoretically predicted and experimentally verified. Sensitive optical gates are realized by varying the feedback phase in both processes.

Physical Review A•Jul 1, 1992•36 citations
Orthogonally polarized optical feedback has been proven to act on the frequency of semiconductor lasers. The coupling of this feedback to a nonlinear filter results in bistability for the frequency of the laser output [Phys. Rev. Lett.94, 173902 (2005)]. This phenomenon opens the way to the development of all-optical devices such as a switch between frequency states of the optical emission. For demonstrating this particular application we use an AsGaAl monomode laser emitting around 852 nm, together with a warm atomic cesium vapor as a resonant filter. The output frequency state of the switch is determined by two different frequencies of a control laser, with each control frequency changing the switch frequency in only one direction.
We analyze the dynamics of semiconductor lasers radiation frequency when these lasers are subject to different conditions of optical feedback, and we demonstrate how it is possible to control the emission frequency using the different configurations explored. In the first system studied a semiconductor laser is fed back with light which polarization is orthogonal to the output polarization, spectrally filtered by a cesium atomic vapor. This system, besides presenting an effective technique to stabilize the laser frequency and reduce the laser linewidth, was the first to exhibit frequency bistable and multistable optical regimes with amplitude practically constant. This unique feature opens the way for applications in all-optical FM logical devices. The bistable and multistable regimes are interpreted through a phenomenological model, and, for the bistable regime, we discuss a rate equation model, built taking in account thermal effects and gain saturation. We also present an all-optical frequency switch, the first of his kind. The second system is used to investigate the behavior of the emission frequency of a semiconductor laser with an external cavity, inside which is placed an atomic filter. For different values of the injection current we observe the laser frequency locking in the atomic line, bistability and reproducible frequency instabilities.
Optical feedback with orthogonal polarization enables frequency sweep of semiconductor lasers and leads to frequency bistability when a resonant medium is used to filter the reinjected radiation. Here, we explore a configuration with two lasers coupled through mutual injection. Each laser injects and receives light with a polarization orthogonal to the plane of emission. Both injections are independently filtered by a resonant atomic vapor. We show that this more versatile version also exhibits bistable states, and that it is possible to reduce the laser frequency jitter as well as to invert its frequency hysteresis cycle on demand (from counterclockwise to clockwise and vice versa). Experimental demonstration is done with diode lasers emitting around 780 nm, using Rb thermal vapors as nonlinear filters.
Traditional frequency domain optical bistability(FDOB) devices with hybrid electro-optical feedback have low response speed and high noise fluctuations.Hence,a novel tunable laser FDOB device with an all-optical feedback was developed using a nonlinear fiber ring resonator as the frequency feedback element.Parametric equations of optical bistability were established according to the system's response to nonlinear process and frequency-dependent feedback.Based on the parametric equations,the characteristics and controllable operations of FDOB were analyzed.The switching response speed of the optical bistability was discussed.The analysis showed that the proposed all-fiber laser bistability device can effectively achieve intensity-driven and gain-driven optical bistability.The position and shape of the bistability hysteresis curve vary with the adjustment of gain or loss in the fiber ring resonator,hence realizing the controlled all-optical bistability operations.Sudden jumping of optical bistability in the frequency domain can be applied to monitor laser wavelength shift and achieve sensoring.The optical bistability response time is in the nanosecond order of magnitude and bistability switching is ultrafast.
The basic mechanisms of the polarization switching in vectorial bistable lasers are studied both theoretically and experimentally versus internal parameters. In particular, by scanning the frequency of a gas laser with two linearly polarized eigenstates, two quite different flipping processes with hysteresis occur according to the linear-phase-anisotropy value of the cavity. Indeed, when the anisotropy increases, rotation and inhibition mechanisms appear successively. The variations of the hysteresis loop for different anisotropy and excitation values are theoretically found to be opposed in the two processes. Additional evolutions of the polarization, such as multiple switchings in the inhibition mechanism and ``hybrid'' hysteresis loops, are predicted. The experiments, essentially performed on a monomode 3.39-\ensuremath{\mu}m $^{3}\mathrm{\ensuremath{-}}^{20}$Ne laser containing an adjustable linear phase anisotropy, confirm the existence of the two processes and their corresponding properties. These processes may also occur in other quasi-isotropic lasers versus other internal parameters, such as, for instance, the injection current in semiconductor lasers. In this case the TE and TM modes flip only in the inhibition mechanism when the bistability conditions are satisfied. The knowledge of the basic flipping mechanisms in the laser itself enables us to understand and realize the external optical-polarization control by an anisotropic feedback (one-frequency systems). Induced-rotation and induced-inhibition mechanisms are then theoretically predicted and experimentally verified. Sensitive optical gates are realized by varying the feedback phase in both processes.