• Photonics Research
  • Vol. 6, Issue 5, B37 (2018)
Samuel Serna1、2、*, Hongtao Lin3, Carlos Alonso-Ramos1, Anupama Yadav4, Xavier Le Roux1, Kathleen Richardson4, Eric Cassan1, Nicolas Dubreuil2, Juejun Hu3, and Laurent Vivien1
Author Affiliations
  • 1Centre de Nanosciences et de Nanotechnologies (C2N), CNRS, Univ. Paris-Sud, Université Paris Saclay, C2N Orsay, 91405 Orsay cedex, France
  • 2Laboratoire Charles Fabry, Institut d’Optique Graduate School, CNRS, Université Paris Saclay, 2 Avenue Augustin Fresnel, 91127 Palaiseau cedex, France
  • 3Department of Materials Science and Engineering, Massachusetts Institute of Technology-MIT, Cambridge, Massachusetts 02139, USA
  • 4College of Optics and Photonics-CREOL, University of Central Florida, Orlando, Florida 32816, USA
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    DOI: 10.1364/PRJ.6.000B37 Cite this Article Set citation alerts
    Samuel Serna, Hongtao Lin, Carlos Alonso-Ramos, Anupama Yadav, Xavier Le Roux, Kathleen Richardson, Eric Cassan, Nicolas Dubreuil, Juejun Hu, Laurent Vivien. Nonlinear optical properties of integrated GeSbS chalcogenide waveguides[J]. Photonics Research, 2018, 6(5): B37 Copy Citation Text show less

    Abstract

    In this paper, we report the experimental characterization of highly nonlinear GeSbS chalcogenide glass waveguides. We used a single-beam characterization protocol that accounts for the magnitude and sign of the real and imaginary parts of the third-order nonlinear susceptibility of integrated Ge23Sb7S70 (GeSbS) chalcogenide glass waveguides in the near-infrared wavelength range at λ=1580 nm. We measured a waveguide nonlinear parameter of 7.0±0.7 W 1·m 1, which corresponds to a nonlinear refractive index of n2=(0.93±0.08)×10 18 m2/W, comparable to that of silicon, but with an 80 times lower two-photon absorption coefficient βTPA=(0.010±0.003) cm/GW, accompanied with linear propagation losses as low as 0.5 dB/cm. The outstanding linear and nonlinear properties of GeSbS, with a measured nonlinear figure of merit FOMTPA=6.0±1.4 at λ=1580 nm, ultimately make it one of the most promising integrated platforms for the realization of nonlinear functionalities.
    ANL=(Re[e×h*]·zd2r)2ϵ02c2SNLn02|e|4d2r,(1)

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    ϕNL(1,2)=k0n2ANLPp(1,2)Leff=γwgκinj(1,2)κ(FA,FB)ηPinLeff,(2)

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    PinPout=βTPAηLeffANLκFBκOSA(1)eαLPin+1κFAκFBκOSA(1)eαL=bPin+a,(3)

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    βTPA=baANLκFAηLeff,(4)

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    Samuel Serna, Hongtao Lin, Carlos Alonso-Ramos, Anupama Yadav, Xavier Le Roux, Kathleen Richardson, Eric Cassan, Nicolas Dubreuil, Juejun Hu, Laurent Vivien. Nonlinear optical properties of integrated GeSbS chalcogenide waveguides[J]. Photonics Research, 2018, 6(5): B37
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