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Giant Non-resonant Infrared Second Order Nonlinearity in γ-NaAsSe₂

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arxiv 2111.13725 v1 pith:WJZSJMVL submitted 2021-11-26 physics.optics cond-mat.mtrl-sci

Giant Non-resonant Infrared Second Order Nonlinearity in γ-NaAsSe₂

classification physics.optics cond-mat.mtrl-sci
keywords gammainfraredbandgapcrystalsnaasseapplicationscoefficientsdevices
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Infrared laser systems are vital for applications in spectroscopy, communications, and biomedical devices, where infrared nonlinear optical (NLO) crystals are required for broadband frequency down-conversion. Such crystals need to have high non-resonant NLO coefficients, a large bandgap, low absorption coefficient, phase-matchability among other competing demands, e.g., a larger bandgap leads to smaller NLO coefficients. Here, we report the successful growth of single crystals of $\gamma$-NaAsSe$_2$ that exhibit a giant second harmonic generation (SHG) susceptibility of d$_{11}$=590 pm V$^{-1}$ at 2$\mu$m wavelength; this is ~ eighteen times larger than that of commercial AgGaSe$_2$ while retaining a similar bandgap of ~1.87eV, making it an outstanding candidate for quasi-phase-matched devices utilizing d$_{11}$. In addition, $\gamma$-NaAsSe$_2$ is both Type I and Type II phase-matchable, and has a transparency range up to 16$\mu$m wavelength. Thus $\gamma$-NaAsSe2 is a promising bulk NLO crystal for infrared laser applications.

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