2016
DOI: 10.1016/j.nima.2016.10.008
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Inverse Compton scattering X-ray source yield optimization with a laser path folding system inserted in a pre-existent RF linac

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Cited by 7 publications
(6 citation statements)
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“…But, the minimal time spacing of 15 ns between each γ-ray pulse required for the GBS ruled out this optical configuration for the interaction point. Multi-pass non-resonant cavity studies have been carried out for inverse Compton scattering source [17][18][19][20] and have shown to be adapted to low number of bunches and tens of nanoseconds circulation period. The multi pass non-resonant cavity or laser beam circulator designed for the GBS has got the particularity to achieve constant interaction parameter (angle, waist, polarization) at a fixed interaction point all along the passes.…”
mentioning
confidence: 99%
“…But, the minimal time spacing of 15 ns between each γ-ray pulse required for the GBS ruled out this optical configuration for the interaction point. Multi-pass non-resonant cavity studies have been carried out for inverse Compton scattering source [17][18][19][20] and have shown to be adapted to low number of bunches and tens of nanoseconds circulation period. The multi pass non-resonant cavity or laser beam circulator designed for the GBS has got the particularity to achieve constant interaction parameter (angle, waist, polarization) at a fixed interaction point all along the passes.…”
mentioning
confidence: 99%
“…• Combining a warm s-band linac and a pulsed laser: a 30 keV, femtosecond x-ray beam was generated with a 90 • cross-angle at Berkeley National Laboratory [280]; a very high peak flux x-ray beam (2 × 10 9 up to 10 10 ph/pulse) was produced at Vanderbilt University [281]; a 52 keV x-ray beam was generated at Tsinghua University, China with controllable polarization [282,283]; and an 11 keV x-ray beam was produced at CEA, France, by utilizing a ring-down laser cavity with a folded laser path [284]; • With a linac FEL: tunable 7 to 12 keV x-rays were demonstrated at CLIO, France, using an infrared linac FEL powered by the same electron beam [285]; • With a superconducting linac: a tunable 3.5 to 18 keV, high average flux (few 10 9 ph/s)…”
Section: Compton X-ray Sourcesmentioning
confidence: 99%
“…Various optical systems have been used to increase the available laser beam intensity in Compton scattering experiments. Firstly, 'recirculator' systems [350] have demonstrated effective laser beam energy gains with an enhancement factor between 8 [284] and 20 [351] (an enhancement factor of about 30 is foreseen in reference [352]). Secondly, a FP cavity (optical resonator), a well-known optical device [353][354][355], can provide gain in excess of 10 3 .…”
Section: Photon Beam Systemsmentioning
confidence: 99%
“…Fabry-Perot cavities (FPCs) [1] in the pulsed regime have high-power applications in high harmonic generation [2,3], polarized positron generation [4], and x-or γ-ray production by Compton scattering [5][6][7][8][9][10][11][12][13][14][15][16][17][18]. In this article, we focus on the latter application.…”
Section: Introductionmentioning
confidence: 99%
“…In this article, we focus on the latter application. Most Compton sources are made either of a linear accelerator (linac), coupled to an optical circulator [5][6][7] or a single laser pulse; or a storage ring to a FPC [8][9][10][11][12]. However, for operation in small areas, e.g.…”
Section: Introductionmentioning
confidence: 99%