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

Dunn et al., 2021 - Google Patents

Optical parametric oscillators

Dunn et al., 2021

View PDF
Document ID
2249793581872946955
Author
Dunn M
Ebrahimzadeh M
Publication year
Publication venue
Advances in Lasers and Applications

External Links

Snippet

The basic principles behind the operation of optical parametric oscillators (OPOs) have been known since the early days of nonlinear optics, and many different configurations were explored by the early investigators. The sum of the momenta of the signal and idler photons …
Continue reading at opg.optica.org (PDF) (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
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/106Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity
    • H01S3/108Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity using a non-linear optical device, e.g. exhibiting Brillouin- or Raman-scattering
    • H01S3/109Frequency multiplying, e.g. harmonic generation
    • 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
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/106Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity
    • H01S3/108Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity using a non-linear optical device, e.g. exhibiting Brillouin- or Raman-scattering
    • H01S3/1083Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity using a non-linear optical device, e.g. exhibiting Brillouin- or Raman-scattering using parametric generation
    • 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
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/106Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity
    • H01S3/1063Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity using a solid state device provided with at least one potential jump barrier
    • 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
    • G02F1/353Frequency conversion, i.e. wherein a light beam with frequency components different from those of the incident light beams is generated
    • G02F1/3544Particular phase matching techniques
    • G02F2001/3548Quasi-phase-matching [QPM], e.g. using a periodic domain inverted structure
    • 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
    • H01S3/08Construction or shape of optical resonators or components thereof
    • H01S3/08018Mode suppression
    • H01S3/08022Longitudinal mode control, e.g. specifically multimode
    • H01S3/08031Single-mode emission
    • 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
    • H01S3/08Construction or shape of optical resonators or components thereof
    • H01S3/081Construction or shape of optical resonators or components thereof comprising more than two reflectors
    • 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
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/11Pulse generation, e.g. Q-switching, mode locking
    • H01S3/1106Mode locking
    • H01S3/1112Passive mode locking
    • H01S3/1115Passive mode locking using a saturable absorber
    • 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
    • H01S3/07Construction or shape of active medium consisting of a plurality of parts, e.g. segments
    • 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
    • H01S3/0941Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode
    • H01S3/09415Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping

Similar Documents

Publication Publication Date Title
US8477410B2 (en) Optical parametric oscillator pumped by femtosecond thin-disk laser
Ebrahimzadeh et al. Optical parametric oscillators
Ebrahimzadeh Mid-infrared ultrafast and continuous-wave optical parametric oscillators
US7433373B2 (en) Actively Q-switched laser system using quasi-phase-matched electro-optic Q-switch
Scheidt et al. Diode-laser-pumped continuous-wave KTP optical parametric oscillator
Vodopyanov Pulsed mid-IR optical parametric oscillators
WO1998001927A1 (en) Optical parametric oscillator
Dunn et al. Optical parametric oscillators
Edwards et al. High-power, continuous-wave, singly resonant, intracavity optical parametric oscillator
Henderson et al. Doubly-resonant optical parametric oscillators: tuning behaviour and stability requirements
Ebrahim-Zadeh Mid-infrared optical parametric oscillators and applications
Ebrahimzadeh et al. Temperature‐tuned noncritically phase‐matched picosecond LiB3O5 optical parameter oscillator
Bäder et al. Optical parametric oscillator of quasi-phasematched LiNbO3 pumped by a compact high repetition rate single-frequency passively Q-switched Nd: YAG laser
US8649404B2 (en) Compact and efficient visible laser source with high speed modulation
Sarrouf et al. Intracavity second-harmonic generation of diode-pumped continuous-wave, single-frequency 1.3 µm Nd: YLiF4 lasers
Koch et al. Narrow-band, tunable 2 μm optical parametric oscillator based on MgO: PPLN at degeneracy with a volume Bragg grating output coupler
Simon et al. Nonlinear optical frequency conversion techniques
Mekteplioglu et al. Broadly tunable (402–535 nm) intracavity frequency-doubled Cr: LiSAF laser
Myers et al. CW singly resonant optical parametric oscillators based on 1.064-um pumped periodically poled LiNbO3
Pasiskevicius et al. Low-threshold midinfrared optical parametric oscillation in periodically poled KTiOPO4
Yang et al. Cascaded Mode-Locked Nd: YVO 4 Laser Using MgO Doped Periodically-Poled LiNbO 3 With Direct In-Band Diode Pumping at 914 nm
Grayson et al. Synchronous pumping of a periodically poled LiNbO3 optical parametric oscillator
Wallenstein Advanced solid state sources for high power visible light generation
Simon et al. expanding the dipole moment per unit volume P in a Taylor series in terms of the incident oscillating electrical field [1]: P= ɛ (y E+ 7 EE+ y EEE+---).(1) where y is the weakly dispersive dielectric susceptibility; ɛ, is the vacuum perme
WO2020056655A1 (en) Near-infrared laser and laser generation method