• Photonics Research
  • Vol. 6, Issue 2, 138 (2018)
Liping Gong1, Bing Gu1、*, Guanghao Rui1, Yiping Cui1, Zhuqing Zhu2, and Qiwen Zhan3
Author Affiliations
  • 1Advanced Photonics Center, Southeast University, Nanjing 210096, Jiangsu, China
  • 2Key Laboratory of Optoelectronic Technology of Jiangsu Province, School of Physical Science and Technology, Nanjing Normal University, Nanjing 210023, Jiangsu, China
  • 3Department of Electro-Optics and Photonics, University of Dayton, 300 College Park, Dayton, Ohio 45469-2951, USA
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    DOI: 10.1364/PRJ.6.000138 Cite this Article Set citation alerts
    Liping Gong, Bing Gu, Guanghao Rui, Yiping Cui, Zhuqing Zhu, Qiwen Zhan. Optical forces of focused femtosecond laser pulses on nonlinear optical Rayleigh particles[J]. Photonics Research, 2018, 6(2): 138 Copy Citation Text show less

    Abstract

    The principle of optical trapping is conventionally based on the interaction of optical fields with linear-induced polarizations. However, the optical force originating from the nonlinear polarization becomes significant when nonlinear optical nanoparticles are trapped by femtosecond laser pulses. Herein we develop the time-averaged optical forces on a nonlinear optical nanoparticle using high-repetition-rate femtosecond laser pulses, based on the linear and nonlinear polarization effects. We investigate the dependence of the optical forces on the magnitudes and signs of the refractive nonlinearities. It is found that the self-focusing effect enhances the trapping ability, whereas the self-defocusing effect leads to the splitting of the potential well at the focal plane and destabilizes the optical trap. Our results show good agreement with the reported experimental observations and provide theoretical support for capturing nonlinear optical particles.
    E(r,t)=E0(r)exp(iωt)exp[2(ln2)t2/τF2],(1)

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    B(r,t)=1iω×E(r,t),(2)

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    p(r,t)=αe(r,t)1iαe(r,t)k3/(6πϵ0)E(r,t),(3)

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    αe(r,t)=4πϵ0a3(χ1+χ3|E(r,t)|2)χ1+χ3|E(r,t)|2+3,(4)

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    F=14TT/2T/2[(p+p*)·(E+E*)+(pt+p*t)×(B+B*)]dt,(5)

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    F=πϵ0a3τFνln2Re[β(E0·E0*+E0××E0*)],(6)

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    β=(χ1+χ3|E0|2eζ2)eζ23+(12ik3a3/3)(χ1+χ3|E0|2eζ2)dζ.(7)

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    F=14Re(α)|E0|2+kϵ0cIm(α)SOrb,(8)

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    SOrb=S+ϵ0c2kIm[(E0*·)E0],(9)

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    S=12μ0ωIm[E0×(×E0*)],(10)

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    α=πτFν2ln2(γL+γNL),(11)

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    γL=α01iα0k3/(6πϵ0),(12)

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    α0=4πϵ0a3ϵ20/ϵ101ϵ20/ϵ10+2,(13)

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    γNL=12πϵ0a3ηm=2(1)mm1/2(χ3η|E0|2)m1[3+η(ϵ20/ϵ101)]m,(14)

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    η=12ik3a3/3.(15)

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    E0(r)=E00iλ{[I0+cos(2φ)I2]exsin(2φ)I2ey2i cosφI1ez}(16)

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    I0=0ϑl(θ)eikzcosθ(1+cosθ)J0(krsinθ)dθ,(17)

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    I1=0ϑl(θ)sinθeikzcosθJ1(krsinθ)dθ,(18)

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    I2=0ϑl(θ)eikzcosθ(1cosθ)J2(krsinθ)dθ.(19)

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    Liping Gong, Bing Gu, Guanghao Rui, Yiping Cui, Zhuqing Zhu, Qiwen Zhan. Optical forces of focused femtosecond laser pulses on nonlinear optical Rayleigh particles[J]. Photonics Research, 2018, 6(2): 138
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