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MOPML044 |
Start-to-End Beam Dynamic Simulations for PRAE |
495 |
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- A. Vnuchenko
IFIC, Valencia, Spain
- C. Bruni, M. El Khaldi, A. Faus-Golfe, P. Lepercq, C. Vallerand
LAL, Orsay, France
- A. Latina
CERN, Geneva, Switzerland
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The PRAE project (Platform for Research and Applications with Electrons) aims at creating a multidisciplinary R&D facility in the Orsay campus gathering various scientific communities involved in radiobiology, subatomic physics, instrumentation and particle accelerators around an electron accelerator delivering a high-performance beam with energy up to 70 MeV and later 140 MeV, in order to perform a series of unique measurements and future challenging R&D. In this paper we report the first start-to-end simulations from the RF gun, going through the linac and finally to the different experimental platforms. The beam dynamics simulations have been performed using a concatenation of codes. In particular for the linac the RF-Track code recently developed at CERN will be used and benchmarked. The different working points have been analysed in order to minimise the transverse emittance and the beam energy spread including space charge effects at low electron energies.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2018-MOPML044
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TUPML079 |
A Start to End Simulation of the Laser Plasma Wakefield Acceleration Experiment at ESCULAP |
1731 |
SUSPF043 |
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- K. Wang, C. Bruni, K. Cassou, V. Chaumat, N. Delerue, D. Douillet, S. Jenzer, V. Kubytskyi, P. Lepercq, H. Purwar
LAL, Orsay, France
- E. Baynard, M. Pittman
CLUPS, Orsay, France
- J. Demailly, O. Guilbaud, S. Kazamias, B. Lucas, G. Maynard, O. Neveu, D. Ros
CNRS LPGP Univ Paris Sud, Orsay, France
- D. Garzella
CEA, Gif-sur-Yvette, France
- R. Prazeres
CLIO/ELISE/LCP, Orsay, France
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We present a start to end (s2e) simulation of the Laserplasma Wake Field Accelerator (LPWA) foreseen as the ESCULAP project. We use a photo injector to produce a 5 MeV 10 pC electron bunch with a duration of 1 ps RMS, it is boosted to 10 MeV by a S-band cavity and then compressed to 74 fs RMS (30 fs FWHM) by a magnetic compression chicane (dogleg). After the dogleg, a quadrupole doublet and a triplet are utilized to match the Twiss parameters before injecting into the subsequent plasma wakefield. A 40 TW laser is used to excite plasma wakefield in the 10 cm plasma cell. An optimized configuration has been determined yielding at the plasma exit an electron beam at 180 MeV with energy spread of 4.2%, an angular divergence of 0.6 mrad and a duration of 4 fs.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2018-TUPML079
|
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Export • |
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※ LaTeX,
※ Text/Word,
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