Nonlinear Optical Properties of CdSiP<sub>2</sub> Crystal at 1 μm

Cadmium silicon phosphide, CdSiP<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</inf> (CSP), is now recognized as a promising nonlinear optical material for deep-infrared (deep-IR) applications due to its unique properties such as wide transparency range extending from 1-6.6 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu \mathrm{m}$</tex> and high nonlinearity <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(d_{36}\sim 84\ \text{pm}/\mathrm{V})$</tex>. These properties make CSP highly attractive for frequency conversion using the well-established pump laser technology based at 1 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu \mathrm{m}$</tex> to generate deep-Ir radiation at wavelengths as long as 6 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu \mathrm{m}$</tex> [1]. In spite of the high nonlinear gain, the residual linear and nonlinear absorption at <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\sim 1\ \mu \mathrm{m}$</tex> significantly limit the power scaling potential of frequency conversion sources based on CSP. Further, recent commercial availability of high-power femtosecond Yb-fiber lasers emphasize the importance of investigating the nonlinear optical properties of CSP, including two-photon absorption coefficient <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(\beta_{2})$</tex> and nonlinear refractive index <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(n_{2})$</tex> at ~1 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu \mathrm{m}$</tex> pump wavelength, to unlock its full potential of this material as a <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\chi^{(2)}$</tex> nonlinear gain medium.

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Published
2025-06-23
DOI
https://doi.org/10.1109/cleo/europe-eqec65582.2025.11110885
Primary Topic
Nonlinear Optical Materials Studies
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article
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article

Nonlinear Optical Properties of CdSiP2 Crystal at 1 μm

Peter G. Schunemann, S. Chaitanya Kumar, K. T. Zawilski, Bhagirath Singh Chauhan et al.
Nonlinear Optical Materials Studies
article

Nonlinear Optical Properties of CdSiP2 Crystal at 1 μm

Peter G. Schunemann, S. Chaitanya Kumar, K. T. Zawilski, Bhagirath Singh Chauhan, Debashis Pal, M. Ebrahim-Zadeh, Kiran KP
article en

Abstract

Cadmium silicon phosphide, CdSiP<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</inf> (CSP), is now recognized as a promising nonlinear optical material for deep-infrared (deep-IR) applications due to its unique properties such as wide transparency range extending from 1-6.6 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu \mathrm{m}$</tex> and high nonlinearity <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(d_{36}\sim 84\ \text{pm}/\mathrm{V})$</tex>. These properties make CSP highly attractive for frequency conversion using the well-established pump laser technology based at 1 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu \mathrm{m}$</tex> to generate deep-Ir radiation at wavelengths as long as 6 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu \mathrm{m}$</tex> [1]. In spite of the high nonlinear gain, the residual linear and nonlinear absorption at <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\sim 1\ \mu \mathrm{m}$</tex> significantly limit the power scaling potential of frequency conversion sources based on CSP. Further, recent commercial availability of high-power femtosecond Yb-fiber lasers emphasize the importance of investigating the nonlinear optical properties of CSP, including two-photon absorption coefficient <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(\beta_{2})$</tex> and nonlinear refractive index <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(n_{2})$</tex> at ~1 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu \mathrm{m}$</tex> pump wavelength, to unlock its full potential of this material as a <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\chi^{(2)}$</tex> nonlinear gain medium.

Tata Institute of Fundamental Research (IN), Institute of Photonic Sciences (ES), TIFR Centre for Interdisciplinary Sciences (IN), BAE Systems (United States) (US)
Openalex Percentile: Top 79%
Nonlinear Optical Materials Studies
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