• Infrared and Laser Engineering
  • Vol. 51, Issue 7, 20210618 (2022)
Bing Wen1,2, Yangbao Deng1,*, Jiamou Wei2, Saiwen Zhang1..., Depeng Chen1, Shuguang Deng1 and Guangfu Zhang1|Show fewer author(s)
Author Affiliations
  • 1All-solid-state Energy Storage Materials and Devices Key Laboratory of Hunan Province, College of Information and Electronic Engineering, Hunan City University, Yiyang 413000, China
  • 2Key Laboratory for Micro-/Nano-Optoelectronic Devices of Ministry of Education, School of Physics and Electronics, Hunan University, Changsha 410082, China
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    DOI: 10.3788/IRLA20210618 Cite this Article
    Bing Wen, Yangbao Deng, Jiamou Wei, Saiwen Zhang, Depeng Chen, Shuguang Deng, Guangfu Zhang. Supercontinuum generation and manipulation of cosh-Airy pulse in double-zero dispersion medium[J]. Infrared and Laser Engineering, 2022, 51(7): 20210618 Copy Citation Text show less

    Abstract

    Combining the split-step Fourier method with the fourth-order Runge-Kutta integration method, the manipulation and generation of supercontinuum by finite energy cosh-Airy pulses in a double-zero dispersion media was investigated. Firstly, the influences of truncation coefficient a, initial chirp C and distribution factor χ0 on the evolution of cosh-Airy pulses in double-zero dispersion medium were discussed in detail, and the influences of a, C and χ0 on the width of supercontinuum width were statistically analyzed. Then, the influences of higher-order nonlinear effects on supercontinuum generation of cosh-Airy pulse was further studied. The results show that the width of supercontinuum can be controlled by manipulating the characteristic parameters of cosh-Airy pulses. The flatness of supercontinuum is affected with consideration of high-order nonlinear effects. The results provide some theoretical basis for manipulation and generation of supercontinuum and broadband laser sources.
    $ U(Z,T)Z=k2ik+1k!βkkUtk + iγ(1+iω0T)×[U(Z,T) + R(T)|U(Z,TT)|2dT]$(1)

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    $ R\left( T \right) = \left( {1 - {f_R}} \right)\delta \left( T \right){\text{ + }}{f_R}{h_R}\left( T \right) $(2)

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    $ {h_R}\left( T \right) = \frac{{\tau _1^2 + \tau _2^2}}{{{\tau _1}\tau _2^2}}\exp \left( { - \frac{T}{{{\tau _2}}}} \right)\sin \left( { - \frac{T}{{{\tau _1}}}} \right) $(3)

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    $ B\left( {Z,T} \right) = A\left( {Z,T} \right)\exp \left[ {i\gamma \cdot R\left( T \right){{\left| {{A_0}} \right|}^2} \cdot \left( {Z - {Z_0}} \right)} \right] $(4)

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    $ \frac{{\partial B\left( {Z,T} \right)}}{{\partial Z}} = i\gamma B \cdot R\left( T \right) \cdot \left( {{{\left| {{B_0}} \right|}^2} + {{\left| B \right|}^2}} \right) - \frac{\gamma }{{{\omega _0}}} \cdot \left[ {B \cdot R\left( T \right) \cdot {{\left| B \right|}^2}} \right] $(5)

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    $ U\left( {Z = 0,T} \right) = \sqrt {{P_0}} Ai\left( T \right)\exp \left( {aT} \right)\cosh \left( {{\chi _0}T} \right) $(6)

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    $U(Z=0,T)=12[P0Ai(T)exp(a+T)+P0Ai(T)exp(aT)] $(7)

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    $ a+=a+χ0 $(8)

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    $ a=aχ0 $(9)

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    $ U(Z=0,T)=P0Ai(T)exp(aT)exp(iCT2)cosh(χ0T)$(10)

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    $ \sigma _u^2 = \left\langle {{{\left( {T - \left\langle T \right\rangle } \right)}^2}} \right\rangle = \frac{1}{{{P_0}}}{\int_{ - \infty }^{ + \infty } {{{\left( {T - \left\langle T \right\rangle } \right)}^2}\left| A \right|} ^2}{\rm{d}}T $(11)

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    Bing Wen, Yangbao Deng, Jiamou Wei, Saiwen Zhang, Depeng Chen, Shuguang Deng, Guangfu Zhang. Supercontinuum generation and manipulation of cosh-Airy pulse in double-zero dispersion medium[J]. Infrared and Laser Engineering, 2022, 51(7): 20210618
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