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  2. Gain-switching - Wikipedia

    en.wikipedia.org/wiki/Gain-switching

    Gain-switching is a technique in optics by which a laser can be made to produce pulses of light of extremely short duration, of the order of picoseconds (10 −12 s). [ 1 ] [ 2 ] In a semiconductor laser , the optical pulses are generated by injecting many carriers ( electrons ) into the active region of the device, bringing the carrier density ...

  3. Q-switching - Wikipedia

    en.wikipedia.org/wiki/Q-switching

    Q-switching, sometimes known as giant pulse formation or Q-spoiling, [1] is a technique by which a laser can be made to produce a pulsed output beam. The technique allows the production of light pulses with extremely high peak power, much higher than would be produced by the same laser if it were operating in a continuous wave (constant output) mode.

  4. Frequency comb - Wikipedia

    en.wikipedia.org/wiki/Frequency_comb

    A frequency comb or spectral comb is a spectrum made of discrete and regularly spaced spectral lines.In optics, a frequency comb can be generated by certain laser sources.. A number of mechanisms exist for obtaining an optical frequency comb, including periodic modulation (in amplitude and/or phase) of a continuous-wave laser, four-wave mixing in nonlinear media, or stabilization of the pulse ...

  5. Optical spectrometer - Wikipedia

    en.wikipedia.org/wiki/Optical_spectrometer

    In the mid- to far-IR, spectra are typically expressed in units of Watts per unit wavelength (μm) or wavenumber (cm −1). In many cases, the spectrum is displayed with the units left implied (such as "digital counts" per spectral channel). A comparison of the four abscissa types typically used for visible spectrometers.

  6. Resonance-enhanced multiphoton ionization - Wikipedia

    en.wikipedia.org/wiki/Resonance-enhanced_multi...

    In contrast to optical heterodyne techniques, no alignment or mode matching of the reference is necessary. The long wavelength of the microwaves leads to effective point coherent scattering from the plasma in the laser focal volume, so phase matching is unimportant and scattering in the backward direction is strong.

  7. Wavelength-division multiplexing - Wikipedia

    en.wikipedia.org/wiki/Wavelength-division...

    ITU G.694.2 was revised in 2003 to shift the channel centers by 1 nm so, strictly speaking, the center wavelengths are 1271 to 1611 nm. [5] Many CWDM wavelengths below 1470 nm are considered unusable on older G.652 specification fibers, due to the increased attenuation in the 1270–1470 nm bands.

  8. Two-photon absorption - Wikipedia

    en.wikipedia.org/wiki/Two-photon_absorption

    Schematic of energy levels involved in two photons absorption. In atomic physics, two-photon absorption (TPA or 2PA), also called two-photon excitation or non-linear absorption, is the simultaneous absorption of two photons of identical or different frequencies in order to excite an atom or a molecule from one state (usually the ground state), via a virtual energy level, to a higher energy ...

  9. Saturated absorption spectroscopy - Wikipedia

    en.wikipedia.org/wiki/Saturated_absorption...

    Saturated absorption spectroscopy measures the transition frequency of an atom or molecule between its ground state and an excited state.In saturated absorption spectroscopy, two counter-propagating, overlapped laser beams are sent through a sample of atomic gas.

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