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BiBTeX citation export for TU1C2: Evolution of the Inverse Compton Scattering X-ray Source of the ELSA Accelerator

@inproceedings{pires:fls2023-tu1c2,
  author       = {A. Pires and N. Delerue and V. Le Flanchec and R. Rosch and J. Touguet},
  title        = {{Evolution of the Inverse Compton Scattering X-ray Source of the ELSA Accelerator}},
% booktitle    = {Proc. FLS'23},
  booktitle    = {Proc. 67th ICFA Adv. Beam Dyn. Workshop Future Light Sources (FLS'23)},
  eventdate    = {2023-08-27/2023-09-01},
  pages        = {50--53},
  paper        = {TU1C2},
  language     = {english},
  keywords     = {laser, electron, alignment, scattering, cavity},
  venue        = {Luzern, Switzerland},
  series       = {ICFA Advanced Beam Dynamics Workshop},
  number       = {67},
  publisher    = {JACoW Publishing, Geneva, Switzerland},
  month        = {01},
  year         = {2024},
  issn         = {2673-7035},
  isbn         = {978-3-95450-224-0},
  doi          = {10.18429/JACoW-FLS2023-TU1C2},
  url          = {http://jacow.org/fls2023/papers/tu1c2.pdf},
  abstract     = {{The Inverse Compton Scattering (ICS) X-ray source of ELSA accelerator at CEA-DAM, presents an efficient approach for generating X-rays with a compact linac. The source consists of a 30 MeV, 15 ps rms, up to 3 nC electron beam; and a table-top Nd:YAG laser. X-rays are produced in the 10-80 keV range, higher X-ray energies achieved with frequency doubling of the laser. The yield is increased by a factor of 8 thanks to an optical mirror system developed at CEA, folding the laser beam path and accumulating successive laser pulses. We present a new version of the device, with improvement of mechanical constraints management, adjunction of motorized mirrors, and a new imaging system. A Chirped Pulse Amplification (CPA) system was also designed, enabling higher amplification levels without exceeding laser damage threshold. The uniqueness of this CPA system lies in its use of a short wavelength bandwidth, ±250 pm after Self-Phase Modulation (SPM) broadening, and a line density of 1850 lines/mm for the gratings of the compressor. The pulse is stretched with a chirped fiber Bragg grating (CFBG) before amplification in Nd:YAG amplifiers, and compressed by a double pass grating compressor.}},
}