• Matter and Radiation at Extremes
  • Vol. 6, Issue 6, 065901 (2021)
Hiroki Morita1, Tadashi Ogitsu2, Frank R. Graziani2, and Shinsuke Fujioka1
Author Affiliations
  • 1Institute of Laser Engineering, Osaka University, 2-6 Yamada-Oka, Suita, Osaka 565-0871, Japan
  • 2Lawrence Livermore National Laboratory, 7000 East Avenue, Livermore, California 94550, USA
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    DOI: 10.1063/5.0053621 Cite this Article
    Hiroki Morita, Tadashi Ogitsu, Frank R. Graziani, Shinsuke Fujioka. Advanced analysis of laser-driven pulsed magnetic diffusion based on quantum molecular dynamics simulation[J]. Matter and Radiation at Extremes, 2021, 6(6): 065901 Copy Citation Text show less

    Abstract

    Magnetic diffusion plays an important role in inertial confinement fusion with strong magnetic fields. In this paper, we improve a previous analysis of the generation and diffusion of the magnetic field [Morita et al., Phys. Plasmas 25, 094505 (2018)]. For the generation process, we calculate the temporal evolution of the coil current using a self-consistent circuit model. The results show that the peak of the calculated magnetic field is delayed by 1.2 ns compared with that of the incident laser pulse. For the diffusion process, we evaluate the electrical conductivity of warm dense gold over a wide temperature range (300 K–100 eV) by combining the Kubo–Greenwood formula based on a quantum molecular dynamics simulation with the modified Spitzer model. Our simulation shows that the maximum magnetic field (530 T) that penetrates the cone is delayed by 2.5 ns compared with the laser peak. This result is consistent with experiments [Sakata et al., Nat. Commun. 9, 3937 (2018)] that showed that applying a strong magnetic field improved the heating efficiency of fusion fuel.
    CdVdt(t)=Id(t)I(t),

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    V(t)=LdIdt(t)+I(t)R(t),

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    Id(t)=ehILπrL22kBThot1+eV(t)kBThoteeV(t)/kBThot,

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    Thot=5.7ILλL2[(×1015W/cm2)μm2]0.55[keV].

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    0tdte(αt)2=1α0αtdtet2=π2αerf(αt).

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    Eindt=1με×Bindσε(Eback+Eind)Ebackt,

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    Bindt=×(Eind+Eback)Bbackt=×Eind,

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    Eϕ,indn(i,j)=e(σ/ε)Δt[Eϕ,backn1(i,j)+Eϕ,indn1(i,j)]+1e(σ/ε)ΔtσHr,indz(i,j)Hz,indr(i,j)n12.

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    Hr,indn+12(i,j)=Hr,indn12(i,j)+ΔtμEϕ,indnz(i,j)n,

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    Hz,indn+12(i,j)=Hz,indn12(i,j)1rΔtμr[rEϕ,indn(i,j)].

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    σ(ω)=2πe223me2Ωωn,m,k[f(ɛmk)f(ɛnk)]×ψnk||ψmk2δ(ɛnkɛmkω).

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    σ(ω)=σ01+ω2τ2,

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    1πΔe(x/Δ)2.

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    σ(T)=γ(Zion)T3238ZionlnΛ,

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    γ(Zion)=3π321+153Zion2+509Zion64Zion2+345Zion+288.

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    nznenz1=2UzUz1mekBT2π232expIzeffkBT,

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    ΔIz=(z+1)e2λD2+23az2,

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    Eϕn(i,j)=1e(σ/ε)Δtσjϕn1(i,j)+e(σ/ε)ΔtEϕn1(i,j)+1e(σ/ε)ΔtσHrz(i,j)Hzr(i,j)n12.

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    Hiroki Morita, Tadashi Ogitsu, Frank R. Graziani, Shinsuke Fujioka. Advanced analysis of laser-driven pulsed magnetic diffusion based on quantum molecular dynamics simulation[J]. Matter and Radiation at Extremes, 2021, 6(6): 065901
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