• Matter and Radiation at Extremes
  • Vol. 6, Issue 6, 065903 (2021)
Jie Qiu1, Liang Hao1、a), Lihua Cao1、2, and Shiyang Zou1
Author Affiliations
  • 1Institute of Applied Physics and Computational Mathematics, Beijing 100094, China
  • 2HEDPS, Center for Applied Physics and Technology, Peking University, Beijing 100871, China
  • show less
    DOI: 10.1063/5.0062902 Cite this Article
    Jie Qiu, Liang Hao, Lihua Cao, Shiyang Zou. Collective stimulated Brillouin scattering modes of two crossing laser beams with shared scattered wave[J]. Matter and Radiation at Extremes, 2021, 6(6): 065903 Copy Citation Text show less

    Abstract

    In inertial confinement fusion (ICF), overlapping of laser beams is common. Owing to the effective high laser intensity of the overlapped beams, the collective mode of stimulated Brillouin scattering (SBS) with a shared scattered light wave is potentially important. In this work, an exact analytic solution for the convective gain coefficient of the collective SBS modes with shared scattered wave is presented for two overlapped beams based on a linear kinetic model. The effects of the crossing angle, polarization states, and finite beam overlapping volume of the two laser beams on the shared light modes are analyzed for cases with zero and nonzero wavelength difference between the two beams. It is found that all these factors have a significant influence on the shared light modes of SBS. Furthermore, the out-of-plane modes, in which the wavevectors of daughter waves lie in different planes from the two overlapped beams, are found to be important for certain polarization states and especially for obtuse crossing angles. In particular, adjusting the polarization directions of the two beams to be orthogonal to each other or tuning the wavelength difference to a sufficiently large value (of the order of nanometers) are found to be effective methods to suppress the shared light modes of SBS. This work will be helpful for comprehending and suppressing collective SBS with shared scattered waves in ICF experiments.
    ω0α=ωs+ωesα,

    View in Article

    k0α=ks+kesα,

    View in Article

    kes1=k012+ks22k01ks2k01sin12ϑ1,kes2=k022+ks22k02ks2k02sin12ϑ2,

    View in Article

    cosϑ1=k01ksk01ks=cosφscos(θs+θh),cosϑ2=k02ksk02ks=cosφscos(θsθh).

    View in Article

    δnesαn0=γpmαkesα2c22ωpe2a0αas*

    View in Article

    ksas=jωpe24c2α=1,2δnesα*n0a0αe0αns,

    View in Article

    γpm(ωes,kes)=(1+χI)χe1+χI+χe,

    View in Article

    δnes1n0=γpm1kes12c22ωpe2a01ascosφ1,

    View in Article

    δnes2n0=γpm2kes22c22ωpe2a02cosφ2(ascosδ+assinδ)

    View in Article

    ksas=jωpe24c2n0(δnes1a01cosφ1+δnes2a02cosφ2cosδ),

    View in Article

    ksas=jωpe24c2δnes2n0a02cosφ2sinδ,

    View in Article

    sinδ=ns(e01×e02)cosφ1cosφ2.

    View in Article

    ηas=κ1as+κ2cosδ(ascosδ+assinδ),

    View in Article

    ηas=κ2sinδ(ascosδ+assinδ),

    View in Article

    κc2κc(κ1+κ2)+κ1κ2sin2δ=0.

    View in Article

    asas=κ2cosδsinδκcκ2sin2δ.

    View in Article

    ωs=ω01ωa1=ω02ωa2,

    View in Article

    Δω0ω01ω02=ωa1ωa2=cs(ka1ka2).

    View in Article

    2κcκcU22cos2φ1+cos2φ2κcκcU+(cosφ1cosφ2sinδ)2=0,

    View in Article

    maxφsκcκcU=12(1+|cosδpol|),

    View in Article

    cosδpole01e02=cos2θhcos(β1β2)+sin2θhcos(β1+β2).

    View in Article

    tanφsM=tan[(β1β2)/2]sinθh,cosδpol>0,sinθhtan[(β1β2)/2],cosδpol<0.

    View in Article

    Δω04k01cs=cosϑ1+ϑ24sinϑ1ϑ24,

    View in Article

    Jie Qiu, Liang Hao, Lihua Cao, Shiyang Zou. Collective stimulated Brillouin scattering modes of two crossing laser beams with shared scattered wave[J]. Matter and Radiation at Extremes, 2021, 6(6): 065903
    Download Citation