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| Content Provider | IEEE Xplore Digital Library |
|---|---|
| Author | Kalmykov, S.Y. Shadwick, B.A. Davoine, X. |
| Copyright Year | 2013 |
| Description | Author affiliation: DAM, CEA, Arpajon, France (Davoine, X.) || Dept. of Phys. & Astron., Univ. of Nebraska - Lincoln, Lincoln, NE, USA (Kalmykov, S.Y.; Shadwick, B.A.) |
| Abstract | The radiation pressure of a multi-terawatt, sub-100 fs laser pulse propagating in an under-dense plasma causes complete electron cavitation. The resulting electron density “bubble” guides the pulse over many Rayleigh lengths, leaving the background ions unperturbed while maintaining GV/cm-scale accelerating and focusing gradients. The shape of the bubble, and, hence, the wakefield potentials, evolve slowly, in lockstep with the optical driver. This dynamic structure readily traps background $electrons.^{1}$ The electron injection process can thus be controlled by purely optical means.2, 3Sharp gradients in the nonlinear refractive index produce a large frequency red-shift (Δω ~ ω0), localized at the leading edge of the $pulse.^{2,3}$ Negative group velocity dispersion associated with the plasma response compresses the pulse into a relativistic optical shock (ROS). ROS formation slows the pulse (and the bubble), reducing the electron dephasing length and limiting energy $gain.^{4}$ Furthermore, the ponderomotive force due to the ROS causes the bubble to constantly expand, trapping copious unwanted electrons, polluting the electron spectrum with a high-charge, low-energy $tail.^{1,2}$ Here, we demonstrate a new, all-optical approach to compensating for the increase in pulse bandwidth, thereby delaying ROS formation and thus producing high quality, GeV-scale electron beams with 10-TW-class (rather than $PW-class^{4})$ lasers in mm-scale (rather than cm-scale4), highdensity plasmas $(n_{e0}$ > 5 x $10^{18}$ vs. $10^{17}$ $cm^{-3}).$ We show that a negatively chirped drive pulse with an ultra-high (~ 400 nm) bandwidth: extends the electron dephasing length; prevents ROS formation through dephasing; and almost completely suppresses continuous injection. Precise compensation of the nonlinear frequency shift can be achieved using a higher-order chirp extracted from reduced simulation models. ROS formation can be further delayed by using a plasma channel to suppress diffraction of the pulse leading edge, minimizing longitudinal variations in the pulse. Plasma density tapering further delays dephasing, providing an additional boost in beam energy. |
| Starting Page | 1 |
| Ending Page | 1 |
| File Size | 61840 |
| Page Count | 1 |
| File Format | |
| ISBN | 9781467351713 |
| ISSN | 07309244 |
| DOI | 10.1109/PLASMA.2013.6633483 |
| Language | English |
| Publisher | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Publisher Date | 2013-06-16 |
| Publisher Place | USA |
| Access Restriction | Subscribed |
| Rights Holder | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Subject Keyword | Plasmas Charge carrier processes Electron optics Nonlinear optics Optical diffraction Optical refraction Optical variables control |
| Content Type | Text |
| Resource Type | Article |
| Subject | Atomic and Molecular Physics, and Optics Condensed Matter Physics Electrical and Electronic Engineering |
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