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    HGTR-KTP

    Raicol was the first to develop High Gray Track Resistance KTP crystals. Our unique crystal growth recipe enables high power density with KTP’s high SHG coefficient. The gray tracks occur due to induced color centers in the KTP crystal that have broad optical absorption in the visible and near-infrared wavelengths. Gray tracks are generated when a crystal is subjected to high average power pulsed lasers or CW laser irradiation.  The process of the gray track formation is cumulative and leads to deterioration in transparency and harmonic conversion.      

    Overview

    Raicol has pioneered the development of High Gray Track Resistance KTP crystals, setting a benchmark in the field of nonlinear optics. Our innovative crystal growth technique enhances the high power density capabilities of KTP while leveraging its remarkable Second Harmonic Generation (SHG) coefficient.

    Gray tracks in KTP crystals are a consequence of induced color centers, which result in broad optical absorption within the visible and near-infrared wavelengths. These gray tracks typically form when the crystal is exposed to high average power pulsed lasers or continuous wave (CW) laser irradiation. This cumulative process can lead to a deterioration in the crystal’s transparency and its ability to effectively convert harmonics.

    By addressing the challenges posed by gray track formation, Raicol’s High Gray Track Resistance KTP crystals ensure improved durability and performance under high-power laser conditions, making them an optimal choice for advanced laser applications.

    Specifications

    Specification Value
    Aperture Up to 5×5
    Absorption Coefficient <10@1064nm
    <50@532nm
    Length Up to 15 mm
    Flatness Up to λ/10 @633nm
    Perpendicularity <10 arc min.
    Average Power Density 4000 W/cm² @1064
    2500 W/cm² @532
    Laser-Induced Damage Threshold 1,500 MW/cm² @1064 nm, for 10 ns pulses 10 pps
    Parallelism 20 arc sec.
    AR Coating DBAR
    Scratch/Dig 10/5

    Key Features

    • Average output power density at 532 nm up to 5 kW/ cm².
    • Nonlinear coefficient 4 times higher than LBO.
    • Low absorption at visible and near infrared wavelengths.
    • Broad temperature bandwidth.
    • Non-hygroscopic material.
    • Small walk-off and wide angular bandwidth.

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