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Volumn 175, Issue 1, 2009, Pages 49-55

Mechanisms of electron injection into laser wakefields by a weak counter-propagating pulse

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EID: 69149089152     PISSN: 19516355     EISSN: 19516401     Source Type: Journal    
DOI: 10.1140/epjst/e2009-01116-5     Document Type: Article
Times cited : (9)

References (33)
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    • Mangles, S.P.D.1
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    • T.P. Coffey, Phys. Fluids 14, 1402 (1971)
    • J.M. Dawson, Phys. Rev. 113, 383 (1959); T.P. Coffey, Phys. Fluids 14, 1402 (1971)
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    • P. Zhang, et al., Phys. Plasmas 10, 2093 (2003); Phys. Rev. Lett. 91, 225001 (2003)
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    • Phys. Rev. E 69, 016407 (2004)
    • Z.-M. Sheng, et al., Phys. Rev. Lett. 88, 055004 (2002); Phys. Rev. E 69, 016407 (2004)
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    • The plasma wavebreaking usually appears at a few plasma wave wavelengths (depending upon the plasma wave amplitude) behind the driving pulse due to the relativistic effect. See, for example E. Infeld, G. Rowlands, Phys. Rev. Lett. 62, 1122 (1989)
    • The plasma wavebreaking usually appears at a few plasma wave wavelengths (depending upon the plasma wave amplitude) behind the driving pulse due to the relativistic effect. See, for example, H. Xu, Z.-M. Sheng, J. Zhang, Phys. Scr. 74, 673 (2006); E. Infeld, G. Rowlands, Phys. Rev. Lett. 62, 1122 (1989)
    • (2006) Phys. Scr. , vol.74 , pp. 673
    • Xu, H.1    Sheng, Z.-M.2    Zhang, J.3


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