Carleton et al., 2002 - Google Patents
Continuous-wave singly resonant optical parametric oscillator based on periodically-poled RbTiOAsO/sub 4Carleton et al., 2002
- Document ID
- 17125773405083913244
- Author
- Carleton A
- Stothard D
- Ebrahimzadeh M
- Dunn M
- Publication year
- Publication venue
- Summaries of Papers Presented at the Lasers and Electro-Optics. CLEO'02. Technical Diges
External Links
Snippet
Summary from only given. Continuous-wave optical parametric oscillators represent versatile sources of tunable coherent light. An approach to the development of cw singly resonant oscillators (SROs) is the use of intracavity pumping. Here, the OPO is placed …
- 230000003287 optical 0 title abstract description 10
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- G—PHYSICS
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- G02F—DEVICES 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
- G02F1/00—Devices 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
- G02F1/35—Non-linear optics
- G02F1/353—Frequency conversion, i.e. wherein a light beam with frequency components different from those of the incident light beams is generated
- G02F1/3544—Particular phase matching techniques
- G02F2001/3548—Quasi-phase-matching [QPM], e.g. using a periodic domain inverted structure
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- G02F1/00—Devices 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
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- G02F1/353—Frequency conversion, i.e. wherein a light beam with frequency components different from those of the incident light beams is generated
- G02F1/3534—Three-wave interaction, e.g. sum-difference frequency generation
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- G02F1/3558—Poled materials, e.g. with periodic poling; Fabrication of domain inverted structures, e.g. for quasi-phase-matching [QPM]
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- G02F2001/3503—Structural association of optical elements, e.g. lenses, with the nonlinear optical device
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- H01S3/1063—Controlling 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
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- G02F1/00—Devices 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
- G02F1/01—Devices 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 for the control of the intensity, phase, polarisation or colour
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- H—ELECTRICITY
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- 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
- H01S3/305—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 a gas
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- H01S3/094—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
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- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
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