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Anticorrelation between Ion Acceleration and Nonlinear Coherent Structures from Laser-Underdense Plasma Interaction

F. Sylla, A. Flacco, S. Kahaly, M. Veltcheva, A. Lifschitz, G. Sanchez-Arriaga, E. Lefebvre, and V. Malka
Phys. Rev. Lett. 108, 115003 – Published 13 March 2012

Abstract

In laser-plasma experiments, we observed that ion acceleration from the Coulomb explosion of the plasma channel bored by the laser is prevented when multiple plasma instabilities, such as filamentation and hosing, and nonlinear coherent structures (vortices or postsolitons) appear in the wake of an ultrashort laser pulse. The tailoring of the longitudinal plasma density ramp allows us to control the onset of these instabilities. We deduced that the laser pulse is depleted into these structures in our conditions, when a plasma at about 10% of the critical density exhibits a gradient on the order of 250μm (Gaussian fit), thus hindering the acceleration. A promising experimental setup with a long pulse is demonstrated enabling the excitation of an isolated coherent structure for polarimetric measurements and, in further perspectives, parametric studies of ion plasma acceleration efficiency.

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  • Received 22 July 2011

DOI:https://doi.org/10.1103/PhysRevLett.108.115003

© 2012 American Physical Society

Authors & Affiliations

F. Sylla1, A. Flacco1, S. Kahaly1, M. Veltcheva1,2, A. Lifschitz1, G. Sanchez-Arriaga3, E. Lefebvre3, and V. Malka1

  • 1Laboratoire d’Optique Appliquée, ENSTA, CNRS, Ecole Polytechnique, UMR 7639, 91761 Palaiseau, France
  • 2Dipartimento di Fisica “G. Occhialini,” Università degli Studi di Milano-Biccoca, piazza della Scienza 3, 20126 Milan, Italy
  • 3CEA, DAM, DIF, 91297 Arpajon, France

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Issue

Vol. 108, Iss. 11 — 16 March 2012

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Images

  • Figure 1
    Figure 1
    Experimental setup for the interaction of a microjet and a short Ti:sapphire pulse, illuminated by a linearly polarized frequency-doubled probe pulse. (a) Imaging ion spectrometer along the normal to the main beam with a Thomson parabola (B=0.3T) and chevron microchannel plate (MCP). A second ion spectrometer is also set on the laser axis. (b) Nomarski interferometer. (c) Polarimeter using the Faraday rotation effect. For polarigrams R and T, the polarizers are rotated by, respectively, +10 and 10° from the extinction.Reuse & Permissions
  • Figure 2
    Figure 2
    (a),(b) MCP recordings normally to the laser axis for ne1020cm3. (a) Short-plasma gradient 150μm. He+ trace with energy cutoff 250keV. (b) Long-plasma gradient 250μm. (c),(d) Shadowgram at 1 ps after the pulse enters the jet (resolution 1μm, magnification 8.2). (c) Short-plasma gradient. (d) Long-plasma gradient. The shadowgram shows a clear train of bubblelike structures in the laser wake. The laser polarization is normal to the picture (S polarized).Reuse & Permissions
  • Figure 3
    Figure 3
    Time-resolved pulse penetration in the plasma gradient. (a) Reference instant t0, (b) t0+540fs, (c) t0+940fs, (d) t0+1.54ps, and (e) t0+2.84ps. Arrows indicate the growth of prominent laser filaments.Reuse & Permissions
  • Figure 4
    Figure 4
    Spatial distribution of the bubbles for two shots in the same conditions at t0+1.54ps showing (a) antisymmetric (zigzag) and (b) symmetric axial patterns about the main plasma channel.Reuse & Permissions
  • Figure 5
    Figure 5
    (a) Shadowgram with one isolated structure in the laser wake at t0+940fs (τ=350fs, 1019cm3). (b) ϕrot map (in radians) of the yellow square dotted zone in (a). Detuning angle of the polarizers: ±10°. (c) Lineout along the black dotted line in (b).Reuse & Permissions
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