Toolkit/stimulated Brillouin scattering slow light in optical fibers
stimulated Brillouin scattering slow light in optical fibers
Also known as: broadened SBS "slow light" process, SBS slow light process, stimulated Brillouin scattering (SBS) in optical fibers
Taxonomy: Technique Branch / Method. Workflows sit above the mechanism and technique branches rather than replacing them.
Summary
Stimulated Brillouin scattering slow light in optical fibers is an optical-fiber delay method for microwave photonics that provides continuously tunable delay of broadband analog signals. In the cited demonstration, pump-laser chirp control synthesized a broadened SBS response that delayed 1-GHz-wide linear frequency-modulated radio-frequency signals.
Usefulness & Problems
Why this is useful
This method is useful for optically controlled delay of broadband analog radio-frequency signals in microwave photonics. The reported broadened SBS response was designed to provide long delay with low amplitude and phase distortion, addressing signal-fidelity requirements during delay tuning.
Source:
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Problem solved
It addresses the problem of generating continuously tunable delay for GHz-bandwidth analog signals in an optical-fiber platform. The cited work specifically targeted delay of 1-GHz-wide linear frequency-modulated radio-frequency signals of arbitrary carrier frequency.
Source:
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Taxonomy & Function
Primary hierarchy
Technique Branch
Method: A concrete method used to build, optimize, or evolve an engineered system.
Mechanisms
slow-light group delayspectral broadening of the sbs response via pump chirp controlstimulated brillouin scatteringTechniques
No technique tags yet.
Target processes
No target processes tagged yet.
Input: Light
Implementation Constraints
Implementation used stimulated Brillouin scattering in optical fibers and required synthesis of the pump-laser optical spectrum by chirp control to broaden the SBS slow-light response. The available evidence does not provide further construct-level or hardware-level details beyond pump-spectrum engineering in the fiber system.
The supplied evidence is limited to a single 2007 application demonstration in optical fibers. Validation is reported for 1-GHz-wide linear frequency-modulated radio-frequency signals, and the evidence does not establish performance for other signal classes, broader bandwidths, or non-fiber implementations.
Validation
Supporting Sources
Ranked Claims
Stimulated Brillouin scattering slow light in optical fibers was described and demonstrated for continuously tunable delay of broadband analog signals for microwave photonics applications.
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Stimulated Brillouin scattering slow light in optical fibers was described and demonstrated for continuously tunable delay of broadband analog signals for microwave photonics applications.
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Stimulated Brillouin scattering slow light in optical fibers was described and demonstrated for continuously tunable delay of broadband analog signals for microwave photonics applications.
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Stimulated Brillouin scattering slow light in optical fibers was described and demonstrated for continuously tunable delay of broadband analog signals for microwave photonics applications.
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Stimulated Brillouin scattering slow light in optical fibers was described and demonstrated for continuously tunable delay of broadband analog signals for microwave photonics applications.
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Stimulated Brillouin scattering slow light in optical fibers was described and demonstrated for continuously tunable delay of broadband analog signals for microwave photonics applications.
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Stimulated Brillouin scattering slow light in optical fibers was described and demonstrated for continuously tunable delay of broadband analog signals for microwave photonics applications.
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Pump laser chirp control was used to synthesize the optical spectrum and obtain a broadened SBS slow light process with long delay and low amplitude and phase distortions.
The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process, with long delay and low amplitude and phase distortions.
Pump laser chirp control was used to synthesize the optical spectrum and obtain a broadened SBS slow light process with long delay and low amplitude and phase distortions.
The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process, with long delay and low amplitude and phase distortions.
Pump laser chirp control was used to synthesize the optical spectrum and obtain a broadened SBS slow light process with long delay and low amplitude and phase distortions.
The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process, with long delay and low amplitude and phase distortions.
Pump laser chirp control was used to synthesize the optical spectrum and obtain a broadened SBS slow light process with long delay and low amplitude and phase distortions.
The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process, with long delay and low amplitude and phase distortions.
Pump laser chirp control was used to synthesize the optical spectrum and obtain a broadened SBS slow light process with long delay and low amplitude and phase distortions.
The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process, with long delay and low amplitude and phase distortions.
Pump laser chirp control was used to synthesize the optical spectrum and obtain a broadened SBS slow light process with long delay and low amplitude and phase distortions.
The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process, with long delay and low amplitude and phase distortions.
Pump laser chirp control was used to synthesize the optical spectrum and obtain a broadened SBS slow light process with long delay and low amplitude and phase distortions.
The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process, with long delay and low amplitude and phase distortions.
The resulting SBS process delayed 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency, with delays up to 230 ps and a worst-case sidelobe suppression ratio of -26 dB.
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
The resulting SBS process delayed 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency, with delays up to 230 ps and a worst-case sidelobe suppression ratio of -26 dB.
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
The resulting SBS process delayed 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency, with delays up to 230 ps and a worst-case sidelobe suppression ratio of -26 dB.
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
The resulting SBS process delayed 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency, with delays up to 230 ps and a worst-case sidelobe suppression ratio of -26 dB.
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
The resulting SBS process delayed 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency, with delays up to 230 ps and a worst-case sidelobe suppression ratio of -26 dB.
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
The resulting SBS process delayed 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency, with delays up to 230 ps and a worst-case sidelobe suppression ratio of -26 dB.
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
The resulting SBS process delayed 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency, with delays up to 230 ps and a worst-case sidelobe suppression ratio of -26 dB.
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
Approval Evidence
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers. The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process
Source:
Stimulated Brillouin scattering slow light in optical fibers was described and demonstrated for continuously tunable delay of broadband analog signals for microwave photonics applications.
Continuously tunable delay of broadband analog signals for microwave photonics applications is described and demonstrated, based on stimulated Brillouin scattering (SBS) in optical fibers.
Source:
Pump laser chirp control was used to synthesize the optical spectrum and obtain a broadened SBS slow light process with long delay and low amplitude and phase distortions.
The optical spectrum of the pump laser is synthesized using chirp control, in order to obtain a broadened SBS "slow light" process, with long delay and low amplitude and phase distortions.
Source:
The resulting SBS process delayed 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency, with delays up to 230 ps and a worst-case sidelobe suppression ratio of -26 dB.
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
Source:
Comparisons
Source-backed strengths
The reported system achieved delays up to 230 ps for 1-GHz-wide linear frequency-modulated radio-frequency signals. The source also reports low amplitude and phase distortions and a worst-case sidelobe suppression ratio of -26 dB under the demonstrated conditions.
Source:
The resulting SBS process is applied to delay 1-GHz-wide linear frequency modulated radio-frequency signals of arbitrary carrier frequency. Delays up to 230 ps are observed, with a worst-case sidelobe suppression ratio of -26 dB
Ranked Citations
- 1.