Phys. Rev. ST Accel. Beams 6, 041301 (2003) [7 pages]

Modeling of laser wakefield acceleration at CO2 laser wavelengths

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N. E. Andreev, S. V. Kuznetsov, and A. A. Pogosova
Institute for High Energy Densities, Russian Academy of Sciences, Izhorskaya 13/19, Moscow 125412, Russia

L. C. Steinhauer
Redmond Plasma Physics Laboratory, University of Washington, 14700 NE 95th Street, Suite 100, Redmond, Washington 98052, USA

W. D. Kimura *
STI Optronics, Inc., 2755 Northup Way, Bellevue, Washington 98004, USA

Received 4 February 2003; published 29 April 2003

The upgraded Accelerator Test Facility (ATF) CO2 laser located at Brookhaven National Laboratory offers a unique opportunity to investigate laser wakefield acceleration (LWFA) with a 10.6-μm laser, a wavelength where little experimental work exists. While long laser wavelengths have certain advantages over short wavelengths, our modeling analysis has uncovered another important effect. The upgraded ATF CO2 laser will have a pulse length as short as 2 ps. At a nominal plasma density of ∼1016  cm-3, this pulse length would normally be considered too long for resonant LWFA, but too short for self-modulated LWFA. However, our model simulations indicate that a well-formed wakefield is nevertheless generated with electric field gradients of Ez≳2  GV/m assuming 2.5 TW laser peak power. The model indicates pulse steepening is occurring due to various nonlinear effects. It is possible that this intermediate laser pulse length mode of operation may permit the creation of well-formed, regular-shaped wakefields, which would be needed for staging the LWFA process. Discussed in this paper are the model, its predictions for an LWFA experiment at the ATF, and the pulse steepening effect.


©2003 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevSTAB.6.041301
DOI: 10.1103/PhysRevSTAB.6.041301
PACS: 41.75.Jv, 52.38.Kd, 42.55.Lt

* Corresponding author: wkimura@stioptronics.com

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