1990
DOI: 10.1007/bf00665134
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Tunable chromium forsterite laser in the near IR region

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Cited by 18 publications
(2 citation statements)
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“…• Moreover, in the case of Alexandrite, only around 78% of the doped Cr 3+ ions are on laser active sites [83]. As a result, assuming a reasonable inversion level of 25%, in a 0.2% Cr-doped Alexandrite crystal, the ion density in the upper laser level is only around 1.37x10 19 ions/cm 3 (0.25 x 0.2 x 0.78 x 3.51x10 20 ions/cm 3 [49]). The emission cross section of Alexandrite at 765 nm at 100 °C is around 1.3 x10 -20 cm 2 , and neglecting ESA, this results in a small signal gain coefficient (g 0 ) of only around 0.18 cm -1 .…”
Section: Published Bymentioning
confidence: 99%
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“…• Moreover, in the case of Alexandrite, only around 78% of the doped Cr 3+ ions are on laser active sites [83]. As a result, assuming a reasonable inversion level of 25%, in a 0.2% Cr-doped Alexandrite crystal, the ion density in the upper laser level is only around 1.37x10 19 ions/cm 3 (0.25 x 0.2 x 0.78 x 3.51x10 20 ions/cm 3 [49]). The emission cross section of Alexandrite at 765 nm at 100 °C is around 1.3 x10 -20 cm 2 , and neglecting ESA, this results in a small signal gain coefficient (g 0 ) of only around 0.18 cm -1 .…”
Section: Published Bymentioning
confidence: 99%
“…Part of this search is focused on other Yb +3 -doped gain media such as Yb:YLF [8,9], Yb:CALGO [10], and Yb:KYW [11]; however, the emission bandwidth of these materials are also rather limited. As an alternative, transition-metal doped laser materials such as Ti:Sapphire (660-1180 nm) [12][13][14], Alexandrite (701-858 nm) [15][16][17][18][19], Cr:Forsterite (1130-1367) [20,21], Cr:ZnSe (1880-3350 nm) [22,23], etc... provide significantly broader optical gain bandwidth at different regions of the optical spectrum, and investigation of their TD…”
Section: Introductionmentioning
confidence: 99%