3-YB1KGW-01 - Yb(1%):KGW Laser Crystal, 5 x 5 x 2 mm, Ar/AR@980-1080

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3-YB1KGW-01 - Yb(1%):KGW Laser Crystal, 5 x 5 x 2 mm, Ar/AR@980-1080
US$910.00
Yb:KGW and Yb:KYW crystals are used as lasing materials to generate ultrashort high power pulses. Yb:KGW can be used as ultrashort pulses amplifiers and these crystals are one of the best materials for high power thin disk lasers.




The broad spectral emission band of Yb:KYW allows the tuning of the laser radiation over 1020-1060 nm range and the generation of femtosecond pulses shorter than 70 fs. Enhanced storage capacity, wide absorption spectrum at 980 nm and high absorption of pump radiation in a small crystal region allow an efficient use of diode laser pump.




As compared to YAG or glasses used as hosts for Yb3+, KYW and KGdW have the advantage of a larger absorption cross section than YAG, which decreases the minimum pump intensity necessary to achieve transparency in the quasi-two-level system of ytterbium.
Coatings Ar/AR@980-1080
Dimensions, mm 5 x 5 x 2
End surfaces Right-angle cut
Material Yb(1%):KGW
Delivery 2-4 weeks
Description

Details

Yb:KGW and Yb:KYW crystals are used as lasing materials to generate ultrashort high power pulses. Yb:KGW can be used as ultrashort pulses amplifiers and these crystals are one of the best materials for high power thin disk lasers.

The broad spectral emission band of Yb:KYW allows the tuning of the laser radiation over 1020-1060 nm range and the generation of femtosecond pulses shorter than 70 fs. Enhanced storage capacity, wide absorption spectrum at 980 nm and high absorption of pump radiation in a small crystal region allow an efficient use of diode laser pump.

As compared to YAG or glasses used as hosts for Yb3+, KYW and KGdW have the advantage of a larger absorption cross section than YAG, which decreases the minimum pump intensity necessary to achieve transparency in the quasi-two-level system of ytterbium.
Features
  • High absorption coefficient @ 980 nm
  • High stimulated emission cross section
  • Low laser threshold
  • Extremely low quantum defect
  • Broad output at 1020-1060 nm
  • High slope efficiency with diode pumping (>55%)
  • High Yb-doping concentration
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