[go: up one dir, main page]
More Web Proxy on the site http://driver.im/

Chen et al., 2010 - Google Patents

Stimulated Brillouin scattering effect on gain saturation of distributed fiber Raman amplifiers

Chen et al., 2010

Document ID
14837619916635676545
Author
Chen W
Wang K
Meng Z
Publication year
Publication venue
Chinese Optics Letters

External Links

Snippet

Gain saturation is a significant phenomenon of fiber Raman amplifiers (FRAs). Gain figures versus signal power are well explained. For the small signal, the coupled ordinary differential equations are used, and for the large signal, the Raman gain coefficient is …
Continue reading at opg.optica.org (other versions)

Classifications

    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01SDEVICES USING STIMULATED EMISSION
    • H01S3/00Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
    • H01S3/05Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/063Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
    • H01S3/067Fibre lasers
    • H01S3/06754Fibre amplifiers
    • H01S3/06758Tandem amplifiers
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01SDEVICES USING STIMULATED EMISSION
    • H01S3/00Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
    • H01S3/05Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/063Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
    • H01S3/067Fibre lasers
    • H01S3/06708Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
    • H01S3/06729Peculiar transverse fibre profile
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01SDEVICES USING STIMULATED EMISSION
    • H01S3/00Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
    • H01S3/05Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/063Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
    • H01S3/067Fibre lasers
    • H01S3/0675Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS, OR APPARATUS
    • G02B6/00Light guides
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS, OR APPARATUS
    • G02B6/00Light guides
    • G02B6/02Optical fibre with cladding with or without a coating
    • G02B6/036Optical fibre with cladding with or without a coating core or cladding comprising multiple layers
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01SDEVICES USING STIMULATED EMISSION
    • H01S3/00Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
    • H01S3/14Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves characterised by the material used as the active medium
    • H01S3/16Solid materials
    • H01S3/1601Solid materials characterised by an active (lasing) ion
    • H01S3/1603Solid materials characterised by an active (lasing) ion rare earth
    • H01S3/1608Solid materials characterised by an active (lasing) ion rare earth erbium
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01SDEVICES USING STIMULATED EMISSION
    • H01S3/00Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
    • H01S3/30Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves using scattering effects, e.g. stimulated Brillouin or Raman effects
    • H01S3/302Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves using scattering effects, e.g. stimulated Brillouin or Raman effects in an optical fibre
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/29Repeaters
    • H04B10/291Repeaters in which processing or amplification is carried out without conversion of the main signal from optical form
    • H04B10/2912Repeaters in which processing or amplification is carried out without conversion of the main signal from optical form characterised by the medium used for amplification or processing
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01SDEVICES USING STIMULATED EMISSION
    • H01S3/00Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/091Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/094Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
    • H01S3/094003Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light the pumped medium being a fibre

Similar Documents

Publication Publication Date Title
Pinto et al. Multiwavelength Raman fiber lasers using Hi-Bi photonic crystal fiber loop mirrors combined with random cavities
CN102709798B (en) Erbium-doped optical fiber laser for optical fiber grating acoustic emission sensing system
Hu et al. 150-km long distance FBG temperature and vibration sensor system based on stimulated Raman amplification
Chen et al. Stimulated Brillouin scattering effect on gain saturation of distributed fiber Raman amplifiers
Wang et al. Power threshold reduction and laser efficiency improvement of Brillouin fiber laser based on an As2S3 chalcogenide fiber via a mode field adaptor
Lambin-Iezzi et al. Stimulated Brillouin scattering in SM ZBLAN fiber
Jin et al. High-power thulium-doped all-fiber superfluorescent source with ultranarrow linewidth
Li et al. Tunable multiwavelength Brillouin-erbium ring-cavity fiber laser with short-length photonic crystal fiber
Lou et al. High power, high-order random Raman fiber laser based on tapered fiber
CN112033447B (en) Brillouin optical time domain analysis system based on quasi-distributed passive remote pump amplification
Nagel et al. Phosphosilicate Raman gain fibers with varying core concentration for enhanced SBS suppression
Mohd Nasir et al. On the pre-amplified linear cavity multi-wavelength Brillioun-erbium fiber laser with low SBS threshold highly nonlinear photonic crystal fiber
Isoe et al. Noise figure and pump reflection power in SMF-reach optical fibre for Raman amplification
Jin et al. Broadband supercontinuum generation based on ytterbium-doped fiber amplifier seeded by self-pulsed amplified spontaneous emission source
Lu et al. A hybrid fiber amplifier with 36.9-dBm output power and 70-dB gain
Poboril et al. Measuring optimal length of the amplifying fiber in different working conditions of the amplifier
Kale et al. Comparison of SRS & SBS (Non Linear Scattering) In Optical Fiber
Chen et al. Spontaneous and induced modulation instability in the presence of broadband spectra caused by the amplified spontaneous emission
Chi et al. A novel long distance fiber Bragg grating sensor system with low threshold pump power and high OSNR
Ma et al. 3.5 W optical power delivery over 5 km single-mode fiber using C-band amplified spontaneous emission light source
Isoe et al. Noise figure analysis of distributed fibre Raman amplifier
Ran et al. Optimization of ultra-long random fiber lasing sensor
Li et al. Second-order few-mode distributed raman amplifier for mode-division multiplexing transmission
Zhang et al. A model for the enhancement of the gain saturation power of the forward pumped fiber Raman amplifier with the phase modulation
Xu et al. Linearly-polarized narrow-linewidth random fiber laser seeded fiber MOPA