• Chinese Optics Letters
  • Vol. 14, Issue 12, 123201 (2016)
Sandeep Vyas1、*, Takasumi Tanabe2, Manish Tiwari3, and Ghanshyam Singh4
Author Affiliations
  • 1Department of ECE, Vivekananda Institute of Technology (East), Jaipur 303012, India
  • 2Department of EEE, Keio University, Kanagawa 2238521, Japan
  • 3Department of ECE, Manipal University, Jaipur 303007, India
  • 4Department of ECE, Malaviya National Institute of Technology, Jaipur 302017, India
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    DOI: 10.3788/COL201614.123201 Cite this Article Set citation alerts
    Sandeep Vyas, Takasumi Tanabe, Manish Tiwari, Ghanshyam Singh. Chalcogenide photonic crystal fiber for ultraflat mid-infrared supercontinuum generation[J]. Chinese Optics Letters, 2016, 14(12): 123201 Copy Citation Text show less

    Abstract

    In this Letter, we numerically simulate the generation of a 1–15 μm mid-infrared supercontinuum (SC) from a highly nonlinear Ge11.5As24Se64.5-based photonic crystal fiber (PCF). This ultra-broadband SC is achieved in a 100 mm long PCF pumped using 85 fs laser pulses operated at 3.1 μm and a peak pulse power of 3 kW. The proposed design offers a flat dispersion profile with two zero dispersion wavelengths. This broad and flat dispersion profile of the Ge11.5As24Se64.5 PCF, combined with the high nonlinearity (2474 W 1 km 1), generates an ultra-broadband SC.
    Dc(λ)=λcd2neffdλ2,(1)

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    n2(λ)=1+5.78525λ2λ20.287952+0.39705λ2λ230.393382.(2)

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    γ=2πn2λAeff,(3)

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    Aeff=(|E|2dxdy)2|E|4dxdy,(4)

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    Az+α2A(n2βnin+1n!nAtn)=iγ(1+iωot)[A(z,t)R(t)|A(z,tt)|2dt],(5)

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    R(t)=(1fr)δ(t)+frhR(t).(6)

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    gR(f)=2ωpcn2frIm[HR(f)],(7)

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    hR(t)=τ12+τ22τ1τ22exp(tτ2)sin(tτ1).(8)

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    fr=λ2π2n20gR(f)fdf.(9)

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    A(z=0,t)=P0sech(tt0)exp(iC2t2t02),(10)

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    Sandeep Vyas, Takasumi Tanabe, Manish Tiwari, Ghanshyam Singh. Chalcogenide photonic crystal fiber for ultraflat mid-infrared supercontinuum generation[J]. Chinese Optics Letters, 2016, 14(12): 123201
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