• Photonics Research
  • Vol. 12, Issue 4, 774 (2024)
Lihong Hong1、†,*, Yuanyuan Liu2、†, and Zhi-Yuan Li2
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2School of Physics and Optoelectronics, South China University of Technology, Guangzhou 510640, China
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    DOI: 10.1364/PRJ.516105 Cite this Article Set citation alerts
    Lihong Hong, Yuanyuan Liu, Zhi-Yuan Li. Synergic action of linear dispersion, second-order nonlinearity, and third-order nonlinearity in shaping the spectral profile of a femtosecond pulse transporting in a lithium niobate crystal[J]. Photonics Research, 2024, 12(4): 774 Copy Citation Text show less

    Abstract

    We present a detailed theoretical and numerical analysis on the temporal-spectral-spatial evolution of a high-peak-power femtosecond laser pulse in two sets of systems: a pure lithium niobate (LN) plate and a periodically poled lithium niobate (PPLN) plate. We develop a modified unidimensional pulse propagation model that considers all the prominent linear and nonlinear processes and carried out the simulation process based on an improved split-step Fourier transformation method. We theoretically analyze the synergic action of the linear dispersion effect, the second-order nonlinearity (2nd-NL) second-harmonic generation (SHG) effect, and the third-order nonlinearity (3rd-NL) self-phase modulation (SPM) effect, and clarify the physical mechanism underlying the peculiar and diverse spectral broadening patterns previously reported in LN and PPLN thin plate experiments. Such analysis and discussion provides a deeper insight into the synergetic contribution of these linear and nonlinear effects brought about by the interaction of a femtosecond laser pulse with the LN nonlinear crystal and helps to draw a picture to fully understand these fruitful optical physical processes, phenomena, and laws.
    2z2Ei(z,ti)=μ0ε02t2Ei(z,ti)+μ02t2(Pi(1)(z,ti)+Pi(2)(z,ti)+Pi(3)(z,ti)),i=1,2,

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    Ei(z,ti)=Eieff(z,ωi)eiωiti+ik(ωi)z.

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    Pi(1)(z,ti)=dωiPi(1)(z,ωi)eiωiti=dωiε0χ(1)(ωi)Ei(z,ωi)eiωiti+ik(ωi)z=ε0χ(1)(ωi)Eieff(z,ωi)eiωiti+ik(ωi)z,

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    Pi(2)(z,ti)=dωiPi(2)(z,ωi)eiωiti=dωidωjε0χ(2)(ωi,ωj)Ei(z,ωi)eiωiti+ik(ωi)zEj(z,ωj)eiωjtj+ik(ωj)z=ε0χ(2)(ωi,ωj)Eieff(z,ωi)Ejeff(z,ωj)ei(ωiti+ωjtj)ei(k(ωi)+k(ωj))z,

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    Pi(3)(z,ti)=ε0χ(3)|Ei(z,ti)|2Ei(z,ti)=ε0χ(3)Ii(z,ti)Ei(z,ti)=ε0χ(3)Ii(z,ωi)Eieff(z,ωi)eiωiti+ik(ωi)z.

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    ωnormalized=ωω0Δωmax,

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    I(ωi)=I(ωi,t1)+I(ωi,t2)+2I(ωi,t1)I(ωi,t2)cos(Δϕ(ωi)Δϕmax),

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    ΔϕΔϕmax=(2m+1)π,

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    ΔϕΔϕmax=(2m)π

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    Lihong Hong, Yuanyuan Liu, Zhi-Yuan Li. Synergic action of linear dispersion, second-order nonlinearity, and third-order nonlinearity in shaping the spectral profile of a femtosecond pulse transporting in a lithium niobate crystal[J]. Photonics Research, 2024, 12(4): 774
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