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Optical parametric oscillator, OPO

Light sources can either be broadband, such as a Globar, a Nemst glower, an incandescent wire or mercury arc lamp or they can be tunable, such as a laser or optical parametric oscillator (OPO). In the fomier case, a monocln-omator is needed to achieve spectral resolution. In the case of a tunable light source, the spectral resolution is detemiined by the linewidth of the source itself In either case, the spectral coverage of the light source imposes limits on the vibrational frequencies that can be measured. Of course, limitations on the dispersing element and detector also affect the overall spectral response of the spectrometer. [Pg.1162]

The OPA should not be confiised with an optical parametric oscillator (OPO), a resonant-cavity parametric device that is syncln-onously pumped by a femtosecond, mode-locked oscillator. 14 fs pulses, tunable over much of the visible regime, have been obtained by Hache and co-workers [49, with a BBO OPO pumped by a self-mode-locked Ti-sapphire oscillator. [Pg.1972]

Optical parametric oscillators (OPOs) represent another tunable soHd-state source, based on nonlinear optical effects. These have been under development for many years and as of this writing (ca 1994) are beginning to become commercially available. These lasers may be tuned by temperature or by rotating a crystal. Models available cover a broad wavelength range in the visible and infrared portions of the spectmm. One commercial device may be tuned from 410 to 2000 nm. [Pg.12]

Materials for Frequency Doubling. Second-order NLO materials can be used to generate new frequencies through second harmonic generation (SHG), sum and difference frequency mixing, and optical parametric oscillation (OPO). The first, SHG, is given in equation 3. [Pg.137]

Optical parametric oscillator (OPO, see 20) is the real equivalent to the radio frequency shifter however OPO can be replaced by a simple addition of a local oscillator (e.g. laser) through a beam splitter. Multiplication takes place at the level of detectors. For sake of S5mimetry, detectors can be placed at both output of the beam splitter, the intermediate frequency is then the output of the differential amplifier. [Pg.368]

A useful source of continuously tunable radiation from the near UV to the near-IR with unexplored potential in fluorescence studies is the optical parametric oscillator (OPO). These devices have been around since the 1960s(73) and have received a lot of coverage recently in laser and optoelectronic journals/74 This resurgence of interest in OPOs has been brought about by recent improvements in nonlinear crystals and the development of all-solid-state pump-laser sources with the required levels of coherence and intensity. [Pg.400]

The optical parametric oscillator (OPO) is based on the parametric interaction of a strong pump wave with a nonlinear medium that has a highly nonlinear susceptibility. [Pg.68]

An optical parametric oscillator (OPO) was used to select HF(n = 1) in each of the rotational states J = 0—7 in a study of the effect of rotational excitation on the product state distributions in the reaction ... [Pg.125]

IR measurements on doped Si and shown that the subsurface mobile carriers can be probed by their response to an IR near-field with a spatial resolution of 30nm [48]. The group of Havenith presented a scanning near-field infrared microscopy (SNIM) system this is an IR s-SNOM set-up based on a continuous-wave optical parametric oscillator (OPO) as an excitation source with a much wider tunability compared to the usually applied CO2 lasers [49]. With this set-up, a subsurface pattern of implanted gallium ions in a topographically fiat silicon wafer was imaged with a lateral resolution of <30 nm. [Pg.483]

Certain crystals (those in which the unit cell lacks inversion symmetry) enable a variety of useful three-wave mixing processes Second Harmonic Generation (SHG), u>3 = uq + uq Sum Frequency Generation (SFG), uz = uq + w2 Difference Frequency Generation (DFG), u>z — uq — w2 and Optical Parametric Oscillation (OPO), uq = uq + W3. In SHG, for example, energy and momentum (wavevector) conservation requires, for colinear propagation,... [Pg.49]


See other pages where Optical parametric oscillator, OPO is mentioned: [Pg.2962]    [Pg.138]    [Pg.314]    [Pg.337]    [Pg.339]    [Pg.133]    [Pg.343]    [Pg.130]    [Pg.649]    [Pg.537]    [Pg.254]    [Pg.104]    [Pg.111]    [Pg.72]    [Pg.28]    [Pg.285]    [Pg.120]    [Pg.125]    [Pg.73]    [Pg.49]    [Pg.304]    [Pg.6386]    [Pg.6525]    [Pg.314]    [Pg.643]    [Pg.3080]    [Pg.3425]    [Pg.176]    [Pg.268]    [Pg.231]    [Pg.314]    [Pg.2962]    [Pg.6385]   
See also in sourсe #XX -- [ Pg.247 , Pg.252 ]




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OPO (optical parametric oscillation

Optical parametric oscillation

Optical parametric oscillator

Optical parametric oscillators/amplifiers OPOs/OPAs)

Parametric

Parametric oscillation

Parametric oscillator

Parametrization

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