1997
DOI: 10.1016/s0168-9002(97)00539-1
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TESLA FEL photo-injector simulations giving high-quality beams

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Cited by 8 publications
(6 citation statements)
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“…The evaluation of the fields from the phase space coordinates of the particles is done only in the positions instantaneously occupied by the particles. Some codes, as TREDI [15] or ATRAP [16], take into account the effects due to the finite propagation velocity of signals by calculating the fields according to the Lienard-Wiechert formalism,…”
Section: B Integral Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…The evaluation of the fields from the phase space coordinates of the particles is done only in the positions instantaneously occupied by the particles. Some codes, as TREDI [15] or ATRAP [16], take into account the effects due to the finite propagation velocity of signals by calculating the fields according to the Lienard-Wiechert formalism,…”
Section: B Integral Methodsmentioning
confidence: 99%
“…The coordinate z in Eq. (15) (16) represents the radial space charge interaction of a single slice with the whole beam, depending on the instantaneous bunch length and aspect ratio A. The above expression has been derived for a cylindrical beam of homogeneous density.…”
Section: B Integral Methodsmentioning
confidence: 99%
“…We stress here that such high-quality beams are ideal for a wide range of applications, including the injection of electrons in a LINAC accelerator for the production of high energy beams (e.g., in free-electron laser (FEL) experiments which require very low emittances [6]) and the production of ultrashort pulses of x rays with linear and nonlinear Thomson backscattering [12]. …”
Section: Commentsmentioning
confidence: 99%
“…The electron bunches produced so far by the interaction of superintense and ultrashort laser pulses with plasmas, e.g., via laser wakefield acceleration (LWFA) [1] or self-modulated LWFA [2], are characterized by an almost 100% energy spread [3][4][5]. However, in most applications of laser-plasma produced electron bunches (e.g., in the electron injection in a particle accelerator [6] or in the tunable x-ray sources based on the Thomson scattering of an intense laser beam impinging on energetic electron bunches [7,8]), a reduced energy spread and a low transverse emittance of the beam are required. For this reason several teams are presently investigating, with theoretical and experimental approaches, different possibilities of reducing energy spread and beam emittance [9][10][11][12][13].…”
Section: Introductionmentioning
confidence: 99%
“…For a systematic machine design and optimization, it still heavily depends on the use of self-consistent computer simulations. A number of computer codes have been developed in the past years to simulate beam transport inside photoinjectors [3,4,5,6,7,8,9]. As far as we know, a code which can efficiently and accurately handle a three-dimensional beam with large-aspect ratio and large energy spread including possible image-charge effects is still not available on parallel computer.…”
Section: Introductionmentioning
confidence: 99%