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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
File:UndopedCapFig1.gif ...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(1,605 × 622 (75 KB)) - 09:39, 21 June 2013
