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By D. Andreev
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Next-generation electron accelerators with such unique characteristics will be realized using LPA. , 2009; 1996). , 1995). However, the energy spectra of the electron beams were Maxwell-like distributions, and the beam qualities were far from those required for various applications. , 2005). This result is a signiﬁcant step toward the realization of a laser electron accelerator. In this chapter, we provide the overview of the present status of research on LPA. First, we brieﬂy describe the principle of LPA.
Steun et al. Proceedings of EPAC 2006, Edinburgh, Scotland, page 3427. Hol2006 Holldack, K et al. PRL 96, 054801 (2006) Car2009 K. Carva(a), D. Legutand P. M. Oppeneer, EPL, 86 (2009) 57002 Eis2004 S. Eisebitt, J. Lüning, W. F. Schlotter, M. Lörgen, O. Hellwig, W. Eberhardt, and J. Stöhr, Lensless imaging of magnetic nanostructures by X-ray spectro-holography, Nature 432, 885 (2004). Chap2006 H. C. , Nature Phys. 2, 839 (2006) Gun2011 C. Günther, B. Pfau, R. Mitzner, B. Siemer, S. Roling, H. Zacharias, O.
Figures 13(a) and (b) show the electron energy spectra as a function of the position of the laser pulse in no preformed plasma case and preformed plasma case. The spatial evolutions are obtained from the electron energy spectra calculated for the electrons with the angle of the momentum vector with respect to the laser propagation direction in the range of ±50 mrad in the moving window for every 255 time steps. In no preformed plasma case, a clear monoenergetic peak is formed at x ∼ 600 μm and the maximum peak energy reaches ∼ 80 MeV as shown in Fig.