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| < < | High intensity photon beams have various applications in advanced accelerators, from medical imagery (X-rays) to high energy physics (polarized positron beams, photon colliders) passing by nuclear physics (fundamental and applied). They can be obtained by laser-Compton backscattering off electrons, the main advantage being the possibility to produce high flux monochromatic photon beams. In this context, an optical cavity is a unique system to reach the requested laser beam power at high repetition rates. LAL and KEK are developing such light sources and are trying to push forward the technical limits to increase the maximal power stored in these optical cavities. French members : A. Martens, K. Cassou, I. Chaikovska, R. Chiche, K. Dupraz, P. Favier, D. Jehanno, V. Soskov, T. Williams, F. Zomer Japanese members : Y. Honda, S. Araki, M. Fukuda, U. Hosaka, T. Omori, K. Sakaue, T. Takahashi, N. Terunuma, References : [1] J Bonis et al 2012 JINST 7 P01017, http://dx.doi.org/10.1088/1748-0221/7/01/P01017 [2] T Akagi et al 2012 JINST 7 P01021, http://dx.doi.org/10.1088/1748-0221/7/01/P01021 [3] ThomX Technical Design Report, http://hal.in2p3.fr/in2p3-00971281 [4]Chaikovska et al, High flux circularly polarized gamma beam factory: coupling a Fabry-Perot optical cavity with an electron storage ring, Scientific Reports 6, Article number: 36569 (2016) [5]Liu et al, Laser frequency stabilization using folded cavity and mirror reflectivity tuning, Optics Communications 369 (2016) 84–88. | |||||||
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High intensity photon beams have various applications in advanced accelerators, from medical imagery (X-rays) to high energy physics (polarized positron beams, photon colliders) passing by nuclear physics (fundamental and applied). They can be obtained by laser-Compton backscattering off electrons, the main advantage being the possibility to produce high flux monochromatic photon beams. In this context, an optical cavity is a unique system to reach the requested laser beam power at high repetition rates. LAL and KEK are developing such light sources and are trying to push forward the technical limits to increase the maximal power stored in these optical cavities. Alternative operations modes as self-resonating and burst are also studied. French members : A. Martens, L. Amoudry, K. Cassou, D. Nutarelli, R. Chiche, V. Soskov, F. Zomer Japanese members : A. Aryshev, Y. Honda, M. Fukuda, T. Omori, K. Sakaue, T. Takahashi References : [1] J Bonis et al 2012 JINST 7 P01017, http://dx.doi.org/10.1088/1748-0221/7/01/P01017 [2] T Akagi et al 2012 JINST 7 P01021, http://dx.doi.org/10.1088/1748-0221/7/01/P01021 [3] ThomX Technical Design Report, http://hal.in2p3.fr/in2p3-00971281 [4]Chaikovska et al, High flux circularly polarized gamma beam factory: coupling a Fabry-Perot optical cavity with an electron storage ring, Scientific Reports 6, Article number: 36569 (2016) [5]Liu et al, Laser frequency stabilization using folded cavity and mirror reflectivity tuning, Optics Communications 369 (2016) 84–88. | |||||||