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Electron bunch acceleration and trapping by ponderomotive force of an intense short-pulse laser

Published online by Cambridge University Press:  02 June 2005

SHIGEO KAWATA
Affiliation:
Department of Electrical and Electronic Engineering, Utsunomiya University, Utsunomiya, Japan
QING KONG
Affiliation:
Institute of modern physics, Fudan University, Shanghai, China
SHUJI MIYAZAKI
Affiliation:
Department of Electrical and Electronic Engineering, Utsunomiya University, Utsunomiya, Japan
KOHICHI MIYAUCHI
Affiliation:
Department of Electrical and Electronic Engineering, Utsunomiya University, Utsunomiya, Japan
RYO SONOBE
Affiliation:
Department of Electrical and Electronic Engineering, Utsunomiya University, Utsunomiya, Japan
KEI SAKAI
Affiliation:
Department of Electrical and Electronic Engineering, Utsunomiya University, Utsunomiya, Japan
KAZUHISA NAKAJIMA
Affiliation:
High Energy Accelerator Research Organization, Ibaraki, Japan
SHINICHI MASUDA
Affiliation:
High Energy Accelerator Research Organization, Ibaraki, Japan
Y.K. HO
Affiliation:
Institute of modern physics, Fudan University, Shanghai, China
NORIAKI MIYANAGA
Affiliation:
Institute of Laser Engineering Osaka University, Osaka, Japan
JIRI LIMPOUCH
Affiliation:
Institute of Physics and Czech Technical University, Academy of Sciences of the Czech Republic, Praha, Czech Republic
A.A. ANDREEV
Affiliation:
Research Institute for Laser Physics, Scientific Center, “S.I.Vavilov State Optical Institute”, St. Petersburg, Russia

Abstract

Electron ponderomotive acceleration in a vacuum by a short-pulsed laser of TEM (1, 0) + TEM (0, 1) mode is studied in this paper using a 3-dimensional (3D) particle simulation. It was found that the laser can trap electrons in transverse and accelerate them with the longitudinal ponderomotive force at the same time. Through this electron trapping and acceleration scheme of TEM (1, 0) + TEM (0, 1) mode laser, the electron bunch is confined well in transverse and compressed remarkably in longitudinal. Therefore, a high energy, high density, and low emittances electron bunch is generated. For example, the result shows that for a laser with intensity of a0 = eE0 /mωc = 10, the laser spot size of w0 = 15λ, and the laser pulse length of Lz = 10λ, the maximum energy gain reaches 301 MeV and the average energy 57.7 MeV. The electron bunch transverse radius is about 350λ and the longitudinal size about 20λ. The property of this accelerated bunch is improved compared with that generated by the laser of TEM (0, 0) mode.

Type
Research Article
Copyright
2005 Cambridge University Press

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References

REFERENCES

Cao, N., Ho, Y.K., Kong, Q., Wang, P.X., Yuan, X.Q., Nishida, Y., Yugami, N. & Ito, H. (2002). Accurate description of Gaussian laser beams and electron dynamics. Opt. Commun. 204, 715.Google Scholar
Chaloupka, J.L. & Meyerhofer, D.D. (1999). Observation of electron trapping in an intense laser beam. Phys. Rev. Lett. 83, 45384541.CrossRefGoogle Scholar
Davis, L.W. (1979). Theory of electromagnetic beams. Phys. Rev. A. 19, 11771179.CrossRefGoogle Scholar
Esarey, E., Sprangle, P., Pillof, M. & Krall, J. (1995). Theory and group velocity of ultrashort, tightly focused laser pulses. J. Opt. Soc. Am. B 12, 16951703.CrossRefGoogle Scholar
Kawata, S., Maruyama, T., Watanabe, H. & Takahashi, I. (1991). Inverse-Bremsstrahlung Electron Acceleration. Phys. Rev. Lett. 66, 20722075.CrossRefGoogle Scholar
Kibble, T.W.B. (1966). Refraction of electron beams by intense electromagnetic waves. Phys. Rev. Lett. 16, 10541056.CrossRefGoogle Scholar
Kong, Q., Miyazaki, S., Kawata, S., Miyanaga, K., Nakajima, K., Masuda, S., Miyanaga, N. & Ho, Y.K. (2003). Electron bunch acceleration and trapping by the ponderomotive force of an intense short-pulse laser. Phys. Plasmas. 10, 46054678.CrossRefGoogle Scholar
Meiver, L.K., Jr. & Lubin, M.J. (1974). On the question of charged-particle motion in a focused laser field. J. Appl. Phys. 45, 16821687.CrossRefGoogle Scholar
Moore, C.I. (1992). Confinement of electrons to the centre of a laser focus via the ponderomotive potential. J. Mod. Opt. 39, 21712178.CrossRefGoogle Scholar
Mourou, G., Barty, C.P.J. & Perry, M.D. (1998). Ultrahigh-intensity lasers: Physics of the exterme on a tabletop. Phys. Today 51, 2228.Google Scholar
Pommiers, L. & Lefebvre, E. (2003). Simulation of energetic proton emission in laser-plasma interaction. Laser Part. Beams 21, 573581.Google Scholar
Sakami, H. & Mima, K. (2004). Interconnection between hydro and PIC codes for fast ignition simulations. Laser Part. Beams 22, 4144.Google Scholar
Scully, M.O. & Zubairy, M.S. (1991). Simple laser accelerator: Optics and particle dynamics. Phys. Rev. A. 44, 26562663.CrossRefGoogle Scholar
Shorokhov, O. & Pukhov, A. (2004). Ion acceleration in overdense plasma by short pulse laser. Laser Part. Beams 22, 175183.Google Scholar
Strickland, D. & Mourou, G. (1985). Compression of amplified chirped optical pulses. Opt. Commun. 56, 219221.Google Scholar
Stupakov, G.V. & Zolotorev, M.S. (2001). Ponderomotive laser acceleration and focusing in cacuum for generation of attosecond electron bunches. Phys, Rev. Lett. 86, 52745277.CrossRefGoogle Scholar
Tajima, T. & Dawson, J.M. (1979). Laser electron accelerator. Phys. Rev. Lett. 43, 267270.CrossRefGoogle Scholar
Yariv, A. (1985). Optical Electronics. New York: CBS College Publishing.Google Scholar