Pulse self-modulation and energy transfer induced plasma waveguide arrays
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Pulse self-modulation and energy transfer induced plasma waveguide arrays
Pulse self-modulation and energy transfer between two intersecting laser filaments by selfinduced plasma waveguide arrays R. Kupfer, B. Barmashenko and I. Bar Department of Physics, Ben-Gurion University of the Negev 30 μm 200 μm 𝛍𝐦 250 μm 𝛍𝐦 300 μm 𝛍𝐦 𝛍𝐦 Computational physics in the eyes of experimentalists and theorists Ultrafast lasers 1fs = 10-15 sec = 0.000000000000001 sec Peak intensity > 1016 W/cm2 = 10000000000000000 W/cm2 Nonlinear optics • Light interacts with light via the medium • Intensity dependent refractive index • Light can alter its frequency Propagation of ultrafast laser pulses in air 𝐖 Low intensity regime (𝐈 ~ 𝟏𝟎𝟏𝟑 𝐜𝐦𝟐) • Self focusing due to the nonlinear refractive index 𝑛2 • Plasma defocusing due to multiphoton ionization • Long filaments (up to 2 km) • “Intensity clamping” 𝐖 High intensity regime (𝐈 > 𝟏𝟎𝟏𝟖 𝐜𝐦𝟐) • • • High ionization Relativistic self-focusing Relativistic self-induced transparency A. Couairon and A. Mysyrowicz, Phys. Rep. 441, 47(2006). Algorithm description Initialize Particle Position Solve Poisson Equation 𝜌 𝛻2𝜑 = − 𝜀0 𝑬 = −𝛁𝜑 • • Launch a Pulse on the Simulation Edge • • Solve Maxwell's Curl Equations 1 𝛁 𝜇0 The pulse parameters can be controlled: Duration, intensity, spatial and temporal profile, linewidth, angle, waist and wavelength The simulation area is surrounded by a perfectly matched layer. Spectrum analysis using Goertzel algorithm Only numerical assumptions Ei,j 𝝏𝐄 × 𝑩 = 𝜀0 𝜕𝑡 + 𝑱 𝜕𝑩 𝛁 × 𝑬 = − 𝜕𝑡 Calculate Current Density Caused by Particles Motion 𝑱 = 𝑛𝑞𝒗 Jx i+1,j Hi,j Push Particles According to Lorentz force 𝑑𝛾𝑚𝒗 = 𝑞(𝑬 + 𝒗 × 𝑩) 𝑑𝑡 Jy i,j+1 Analyze Spectrum of Outgoing Pulse on the Edge A. Taflove and S. C. Hagness, Computational Electrodynamics: The Finite-Difference Time-Domain Method, 3rd ed., Norwood, MA (2005). Relativistic self-focusing A. Pukhov and J. Meyer-ter-Vehn, Phys. Rev. Lett. 76, 3975 (1996). Simulation parameters: I = 1.5 × 1019 w0 = 3.5 μm W cm2 e , τ = 200 fs, n = 4 × 1025 m3 and Single bubble regime • Ponderomotive force “pushes” electrons forming a region nearly void of electrons (ion channel) behind the laser pulse Pulse position Fast electron beam • The channel exerts an attractive Coulomb force on the blown out electrons causing them to accelerate into the bubble Simulation parameters: I = 1 × 1018 and w0 = 6.7 μm W cm2 e ,τ = 20 fs, n = 1.73 × 1024 m3 • A fast electron beam is formed • Mori and co-workers formulated the condition for this regime: cτ ≤ w0 ≈ 2 a0 ωcp c - speed of light, τ - pulse duration, w0 - waist, a0 normalized vector potential and ωp - plasma density H. Burau et al. IEEE Trans. Plasma. Sci. 38, 2831 (2010). W. Lu, M. Tzoufras, C. Joshi, F. S. Tsung and W. B. Mori, Phys. Rev. ST Accel. Beams 10, 061301 (2007). Objective – spectral and spatiotemporal evolution Comes in: • Pulse duration: 𝜏 = 45 fs • Spectral linewidth: ∆𝜆 ~ 20 nm • Gaussian shaped spectrum ? Comes out: • Pulse duration: Several pulses of ~ 15 fs (splitting) • Spectral linewidth: ∆𝜆 >> 20 nm (broadening) • Raman Stokes and anti-Stokes peaks and supercontinuum generation • Conical emission Objective – energy transfer between intersecting beams Y. Liu, M. Durand, S. Chen, A. Houard, B. Prade, B. Forestiers, and A. Mysyrowic, Phys. Rev. Lett. 105, 055003 (2010). Spectral and temporal evolution 30 μm 30 μm 200 μm 200 μm 𝛍𝐦 250 μm 250 μm 300 μm 𝛍𝐦 300 μm 𝛍𝐦 Simulation parameters: I = 6 × 1016 Simulation parameters: I = 6 × 1016 W cm2 e ,τ = 45 fs, n = 2.1 × 1025 m3 and w0 = 5.3 μm W cm2 e ,τ = 34 fs, n = 2.1 × 1025 m3 and w0 = 5.3 μm 𝛍𝐦 Energy transfer between intersecting beams Conclusions • PIC simulation of the spectral and spatio-temporal evolution of a single pulse in a high density plasma channel, as well as energy transfer between two intersecting pulses • The simulation results were found to be in agreement with previously obtained experimental results • Efficient frequency conversion and energy transfer can be achieved in a compact and simple setup and over very short distances • It is anticipated that this model will be able to simulate laser-plasma interactions even in more complicated geometries and to predict the behavior under different conditions Future work • Characterization of localized surface plasmons in nanoparticle arrays • Second harmonic generation from irradiated solid targets • Raman and Brillouin scattering in liquids