The Basic Principles Of GTR-KTP Crystal
The Basic Principles Of GTR-KTP Crystal
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The crystals are used in health care lasers for strategies such as laser operation, tattoo removing, and pores and skin resurfacing, in which steady and trustworthy laser effectiveness is crucial.
Increased bulk absorption Homes, reducing IR absorption and increasing All round optical performance.
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A compact successful eye-Secure intracavity optical parametric oscillator pumped by a passively Q-switched Nd:YAG laser inside a shared cavity configuration with successful conversion efficiency as large as 51% is presented.
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Q What's green semico... A At present, the working basic principle of environmentally friendly semiconductor laser is to transform 1064nm infrared gentle emitted by infrared semiconductor laser into 532nm eco-friendly light as a result of nonlinear crystallization. Gre
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Its most favored application is like a frequency doubler website utilizing the 1064nm output of the Nd:YAG laser also to deliver 532nm laser. KTP’s Qualities also help it become excellent for electro-optic modulation, optical parametric era.
KTP is an excellent nonlinear crystal, but its grey tracking phenomena limits its use in large repetition price and higher electrical power laser units. CASTECH's GTR-KTP crystal has larger gray tracking resistance in comparison to the typical flux developed KTP crystal.
Like our hydrothermally developed KTP crystals, flux grown KTP crystals also give outstanding homogeneity. Here are several in their certain parameters:
Superior gray monitoring resistance, rendering it perfect for substantial repetition amount and high-ability laser techniques.
GTR-KTP crystals, made with modern producing processes, exhibit substantially larger resistance to grey monitoring and decrease absorption while in the UV and visible locations, creating them ideal for an array of applications such as frequency doubling, parametric oscillation, and laser amplification.
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Successful sub-nanosecond intracavity optical parametric oscillator pumped by using a passively Q-switched Nd:GdVO4 laser