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

Shepherd et al., 1994 - Google Patents

1.9-μm operation of a Tm: lead germanate glass waveguide laser

Shepherd et al., 1994

View HTML
Document ID
4739921818655567236
Author
Shepherd D
Brinck D
Wang J
Tropper A
Hanna D
Kakarantzas G
Townsend P
Publication year
Publication venue
Optics letters

External Links

Snippet

1.9-μm operation of a Tm:lead germanate glass waveguide laser clickable element to expand a topic LOGIN OR CREATE ACCOUNT PRISM SUBMISSION This website uses cookies to deliver some of our products and services as well as for analytics and to provide you a more …
Continue reading at opg.optica.org (HTML) (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
    • H01S3/06708Constructional 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
    • H01S3/14Lasers, 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
    • H01S3/09Processes 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
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS, OR APPARATUS
    • G02B6/00Light guides
    • G02B6/10Light guides of the optical waveguide type
    • G02B6/12Light guides of the optical waveguide type of the integrated circuit kind
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS, OR APPARATUS
    • G02B6/00Light guides
    • G02B6/02Optical fibre with cladding with or without a coating
    • G02B6/02295Microstructured optical fibre
    • G02B6/02314Plurality of longitudinal structures extending along optical fibre axis, e.g. holes
    • GPHYSICS
    • G02OPTICS
    • G02FDEVICES OR ARRANGEMENTS, THE OPTICAL OPERATION OF WHICH IS MODIFIED BY CHANGING THE OPTICAL PROPERTIES OF THE MEDIUM OF THE DEVICES OR ARRANGEMENTS FOR THE CONTROL OF THE INTENSITY, COLOUR, PHASE, POLARISATION OR DIRECTION OF LIGHT, e.g. SWITCHING, GATING, MODULATING OR DEMODULATING; TECHNIQUES OR PROCEDURES FOR THE OPERATION THEREOF; FREQUENCY-CHANGING; NON-LINEAR OPTICS; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating, or modulating; Non-linear optics
    • G02F1/35Non-linear optics
    • G02F2001/3528Non-linear optics for producing a supercontinuum
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS, OR APPARATUS
    • G02B6/00Light guides
    • G02B6/24Coupling light guides
    • 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

Similar Documents

Publication Publication Date Title
Shepherd et al. 1.9-μm operation of a Tm: lead germanate glass waveguide laser
Jackson et al. High-power diode-cladding-pumped Tm-doped silica fiber laser
Snoeks et al. Cooperative upconversion in erbium-implanted soda-lime silicate glass optical waveguides
Kalita et al. Bismuth doped fiber laser and study of unsaturable loss and pump induced absorption in laser performance
Taira et al. Modeling of quasi-three-level lasers and operation of cw Yb: YAG lasers
Jackson et al. High-power 83 W holmium-doped silica fiber laser operating with high beam quality
Lallier et al. Nd: MgO: LiNbO 3 waveguide laser and amplifier
Ohishi et al. Gain characteristics of tellurite-based erbium-doped fiber amplifiers for 1.5-µm broadband amplification
Dianov et al. Three-cascaded 1407-nm Raman laser based on phosphorus-doped silica fiber
Grivas et al. Tunable, continuous-wave Ti: sapphire channel waveguide lasers written by femtosecond and picosecond laser pulses
Sandrock et al. High-power continuous-wave upconversion fiber laser at room temperature
Ososkov et al. Pump-efficient flattop O+ E-bands bismuth-doped fiber amplifier with 116 nm–3 dB gain bandwidth
Jackson et al. Directly diode-pumped holmium fiber lasers
Chartier et al. Growth and low-threshold laser oscillation of an epitaxially grown Nd: YAG waveguide
Alcock et al. Tunable, continuous-wave neodymium-doped monomode-fiber laser operating at 0.900–0.945 and 1.070–1.135 μm
Qiu et al. Generation of watt-level single-longitudinal-mode output from cladding-pumped short fiber lasers
Barnes et al. High-quantum-efficiency Er 3+ fiber lasers pumped at 980 nm
Le Flohic et al. Room-temperature continuous-wave upconversion laser at 455 nm in a Tm 3+ fluorozirconate fiber
Goldberg et al. High-power superfluorescent source with a side-pumped Yb-doped double-cladding fiber
Griebner et al. Efficient laser operation with nearly diffraction-limited output from a diode-pumped heavily Nd-doped multimode fiber
Koopmann et al. Holmium-doped Lu 2 O 3, Y 2 O 3, and Sc 2 O 3 for lasers above 2.1 μm
Sumiyoshi et al. Dual-wavelength continuous-wave cascade oscillation at 3 and 2 µm with a holmium-doped fluoride-glass fiber laser
Sandrock et al. Diode-pumped 1-W Er-doped fluoride glass M-profile fiber laser emitting at 2.8 µm
Jackson et al. High-power and highly efficient diode-cladding-pumped Ho 3+-doped silica fiber lasers
Pulford et al. kW-level monolithic single-mode narrow-linewidth all-solid photonic bandgap fiber amplifier