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• McCumber relation
  ...ctions of absorption and emission of light in the physics of [[solid-state laser]]s ...omega</math>, and let <math>~T~</math> be the effective temperature of the medium. The McCumbner relation is
  16 KB (2,521 words) - 15:13, 17 June 2020
• Active mirror
  [[Image:DiskLaserJPEG.jpg|200px|right|thumb|Fig.1. An optically-pumped disk laser (active mirror).]] <!--[[Image:DiskLaser.png|200px|right|thumb|Fig.1. An optically-pumped disk laser (active mirror).]] !-->
  15 KB (2,320 words) - 14:31, 20 June 2013
• Tania function
  ...scription of intensity of the electromagnetic wave in the idealized [[gain medium]].!--> ...nia function appears as the intensity of light in the informly pumped gain medium, measured in unit of the saturation intensity. Then, its argument has sense
  27 KB (4,071 words) - 18:29, 16 July 2020
• Doya function
  ...nia. Such a model seems to be applied, in particular, for the [[Yb]]-doped laser materials; realistic values for the saturation intensity can be of order of High-power single-mode solid-state laser with a short, wide unstable cavity.
  19 KB (2,778 words) - 10:05, 1 May 2021
• Gain medium
  ...um''' or '''lasing medium''') is the source of optical [[gain]] within a [[laser]]. The gain results from the [[stimulated emission]] of nuclear, electroni [[laser pumping|pump source]].
  9 KB (1,441 words) - 14:33, 20 June 2013
• Singapore 2011
  ==Application of superfunctions in the Laser science== The 7th Laser Ceramics Symposium (7h LCS) is assisted with the
  8 KB (1,147 words) - 18:44, 30 July 2019
• Coherent atomic energetics
  Self-modulation of optical pulses in a Kerr medium and limits of the single-mode approximation. ...re are no mineral deposits of the excimer molecules, nor deposits of other laser media in already excited states;
  10 KB (1,625 words) - 18:44, 30 July 2019
• Absorbing Schroedinger
  ...) and wavenumber of particle before the entry in the absorbing (detecting) medium. ...inaga and D.Kouznetsov. Waveguide Composed of Pinhole Array. Institute for Laser Science, UEC Chofu, Tokyo 182-8585, JAPAN. 2012-10-05 IWLS. (slideshow and
  15 KB (2,070 words) - 18:47, 30 July 2019
• Absorption
  ...wer of wave during its propagation. Usually, absorption is property of the medium, where the wave propagates. ...that determines the decrease of amplitude or intensity of the wave in the medium.
  3 KB (468 words) - 18:26, 30 July 2019
• WrightOmega
  ...light in an idealized hoomgeneous amplifier with simple model of the gain medium; in the dimension-less form that model gives equation (1). [[Category:Laser science]]
  4 KB (610 words) - 10:22, 20 July 2020
• Keller function
  ...ion]] describes the transfer of the pulse in the simple model of the laser medium with unsaturated gain unity. ...expressed in the way, closer to that it appears in the literature on the [[laser science]]
  10 KB (1,479 words) - 05:27, 16 December 2019
• Shoko function
  ...of light in the homogeneous amplifier within the simple kinetics of laser medium. ...nctions may be important tool of analysis of the transfer functions of the laser amplifiers.
  10 KB (1,507 words) - 18:25, 30 July 2019
• Shoka function
  ==Applications in Laser science== ...d describes the evolution of the short pulse of light in a two-level laser medium. Properties and expansions of the [[Shoka function]] are similar to those o
  3 KB (421 words) - 10:23, 20 July 2020
• ArcKeller
  ...sfer function]] at the amplification of short optical pulses in the [[gain medium]] with simple model of kinetics of excitation of the active centers. Then, [[Laser science]]
  4 KB (545 words) - 18:26, 30 July 2019

• File:BouncingRay.png ...han $2L$, but due to the exponential growth of the intensity in the [[gain medium]] the long rays give significant contribution to the depletion of gain. This picture have been presented at Third Laser Ceramics Symposium 2007, Paris – Auditorium Curie – CNRS – 3 rue Mich (440 × 200 (16 KB)) - 09:39, 21 June 2013

• File:MacCumberViFig1.jpg Cross-sections of the new laser medium versus wavelength, reported in series of publications in 2006 (thick curves Efficient diode-pumped Yb:Gd_2 Si O_5 laser. Appl.Phys.Lett. v.88, 221117 (2006) (857 × 448 (58 KB)) - 07:24, 21 June 2020

• File:McCumberRelationActiveCemters.png Active centers of a composite [[laser medium]] in the simplest two-level approximation [[Category:Laser science]] (676 × 362 (19 KB)) - 11:21, 21 June 2013

• File:Perpetualmo.jpg $\rm Yb : Gd_2 Si O_5$ laser. [[Appl. Phys. Lett.]] 88, 221117 (2006). ...not compatible with the [[Second law of thermodynamics]] and makes such a medium suitable material for the [[perpetual motion machine]] of the second kind. (766 × 572 (33 KB)) - 09:38, 21 June 2013

• File:TaniaPlot.png ...the [[Laser science]] in the simplest model of the uniformly pumped [[gain medium]]. [[Category:Laser science]] (807 × 424 (16 KB)) - 09:39, 21 June 2013

• File:UndopedCap.jpg ...ed cap. The undoped layer prevents the internal reflection from the active medium and allows to make the disk wider, with corresponding increase of maximal p |title=High average power scaleable thin-disk laser (2,784 × 1,102 (97 KB)) - 09:39, 21 June 2013

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