Ahmad et al., 2009 - Google Patents
Bidirectional S-band continuous wave operation in a depressed-cladding erbium doped fiber amplifierAhmad et al., 2009
View PDF- Document ID
- 7105840744122891976
- Author
- Ahmad H
- Zulkifli M
- Latif A
- Thambiratnam K
- Harun S
- Publication year
- Publication venue
- J. Optoelectron. Adv. Mater
External Links
Snippet
The Erbium Doped Fiber Amplifier (EDFA) provides a very convenient amplification of signals at 1550 nm in existing single-mode optical fibre networks. The EDFA is based on Er3+ ions which acts as the active component in the optical amplification process. The EDFA …
- 239000000835 fiber 0 title abstract description 185
Classifications
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/06754—Fibre amplifiers
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/0675—Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/06708—Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/091—Processes or apparatus for excitation, e.g. pumping using optical pumping
- H01S3/094—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
- H01S3/094003—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light the pumped medium being a fibre
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/30—Lasers, 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
- H01S3/302—Lasers, 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
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/29—Repeaters
- H04B10/291—Repeaters in which processing or amplification is carried out without conversion of the main signal from optical form
- H04B10/293—Signal power control
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/08—Construction or shape of optical resonators or components thereof
- H01S3/08018—Mode suppression
- H01S3/08022—Longitudinal mode control, e.g. specifically multimode
- H01S3/08031—Single-mode emission
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/14—Lasers, 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
- H01S3/16—Solid materials
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
- H01S5/14—External cavity lasers
- H01S5/146—External cavity lasers using a fiber as external cavity
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS, OR APPARATUS
- G02B6/00—Light guides
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S2301/00—Functional characteristics
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Zhang et al. | Six-wavelength-switchable narrow-linewidth thulium-doped fiber laser with polarization-maintaining sampled fiber Bragg grating | |
| US6374006B1 (en) | Chirped period gratings for raman amplification in circulator loop cavities | |
| US6603593B2 (en) | Optical transmission link including raman amplifier | |
| Chen | Tunable multiwavelength fiber ring lasers using a programmable high-birefringence fiber loop mirror | |
| KR100319748B1 (en) | Wideband multichannel fiber lasers with output power equalization | |
| Liu et al. | Switchable multi-wavelength erbium-doped random distributed feedback fiber laser incorporating two-stage Sagnac filter | |
| CN100539477C (en) | Raman amplifier | |
| Ahmad et al. | Multi-wavelength Bismuth-doped fiber laser in 1.3 µm based on a compact two-mode fiber filter | |
| Ahmad et al. | Generation of multiwavelength bismuth-doped fiber laser based on all-fiber Lyot filter | |
| Emori et al. | Broadband flat-gain and low-noise Raman amplifiers pumped by wavelength-multiplexed high-power laser diodes | |
| Pérez-Herrera et al. | Stability comparison of two ring resonator structures for multiwavelength fiber lasers using highly doped Er-fibers | |
| Al-Mansoori et al. | L-band multiwavelength BEFL with amplified fiber loop mirror | |
| Fernandez-Vallejo et al. | Comparison of the stability of ring resonator structures for multiwavelength fiber lasers using Raman or Er-doped fiber amplification | |
| Ahmad et al. | Bidirectional S-band continuous wave operation in a depressed-cladding erbium doped fiber amplifier | |
| Ahmad et al. | High power dual-wavelength tunable fiber laser in linear and ring cavity configurations | |
| Ahmad et al. | A compact linear-cavity multi-wavelength Brillouin/thulium fiber laser in S/S+-band | |
| Ahmad et al. | Tunable and switchable Brillouin multi-wavelengtháthulium fluoride fiber laser in S/S+ band region | |
| Perez-Herrera et al. | Switchable multi-wavelength erbium-doped fiber laser for remote sensing | |
| Ali et al. | Single-pump multiwavelength hybrid Raman-EDF laser using a non-adiabatic microfiber interferometer | |
| Kim et al. | Wideband multiwavelength erbium-doped fiber ring laser | |
| Ummy et al. | Tunable multi-wavelength SOA based linear cavity fiber laser source for optical communications applications | |
| Latif | The Generation of Dual-Wavelength Fiber Lasers and their Applications | |
| Ahmad et al. | Tunable S-band multiwavelength Brillouin fiber laser for beat frequency generation at 11 and 22 GHz | |
| Ahmad et al. | Controllable wavelength channels for multiwavelength Brillouin Bismuth/Erbium based fiber laser | |
| Hassan | Ultra-Wideband Soa Fibre Laser |