Difference between revisions of "File:DiskLaserScalingLimit01.jpg"

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Upper bound of the loss $\beta$, at which the putput power $P_{\rm s}$ of an [[active mirror]] is still achievable, versus normalized power $s$, by
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<ref name="ase">{{cite journal| author=D.Kouznetsov| coauthors=J.F.Bisson| title=Role of undoped cap in the scaling of thin-disk lasers| url=http://www.opticsinfobase.org/abstract.cfm?URI=josab-25-3-338| journal=[[JOSAB]]
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|volume=25
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|pages=338–345
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|year=2008| doi=10.1364/JOSAB.25.000338}}</ref>.
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Thick dashed line corresponds to uncovered disk laser; thick solid curve is the same for the disk wuth undoped layer (anti-ASE cap). Thin solid line represents the simplest rough estimate <math> \beta=s^{1/3}</math> without coefficients, which applies to both cases. Circles correspond to various experimental data.
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Copyleft 2007 by Dmitrii Koznetsov. This image may be used for free, attribute <br>
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http://www.ils.uec.ac.jp/~dima/PAPERS/2007josacap.pdf <or>
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http://tori.ils.uec.ac.jp/PAPERS/2007josacap.pdf <or>
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==References==
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<references/>
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[[Category:Laser science]]
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[[Category:Solid state lasers]]
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[[Category:Schemas]]

Latest revision as of 09:39, 21 June 2013

Upper bound of the loss $\beta$, at which the putput power $P_{\rm s}$ of an active mirror is still achievable, versus normalized power $s$, by [1].

Thick dashed line corresponds to uncovered disk laser; thick solid curve is the same for the disk wuth undoped layer (anti-ASE cap). Thin solid line represents the simplest rough estimate \( \beta=s^{1/3}\) without coefficients, which applies to both cases. Circles correspond to various experimental data.

Copyleft 2007 by Dmitrii Koznetsov. This image may be used for free, attribute
http://www.ils.uec.ac.jp/~dima/PAPERS/2007josacap.pdf <or> http://tori.ils.uec.ac.jp/PAPERS/2007josacap.pdf <or>

References

  1. http://www.opticsinfobase.org/abstract.cfm?URI=josab-25-3-338 D.Kouznetsov, J.F.Bisson. Role of undoped cap in the scaling of thin-disk lasers JOSAB 25 p.338–345 (2008)

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