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Author: L. Serafini


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Reference
M. K. Weikum et al., “Status of the Horizon 2020 EuPRAXIA Conceptual Design Study”, in Proc. 10th Int. Particle Accelerator Conf. (IPAC'19), Melbourne, Australia, May 2019, pp. 3638-3642.
D. Sertore et al., “Photocathode Stress Test Bench at INFN LASA”, in Proc. 12th Int. Particle Accelerator Conf. (IPAC'21), Campinas, Brazil, May 2021, pp. 1413-1415.
M. Rossetti Conti et al., “Arc Compressor Test in a Synchrotron - the ACTIS Project”, in Proc. 13th Int. Particle Accelerator Conf. (IPAC'22), Bangkok, Thailand, Jun. 2022, pp. 473-476.
I. Drebot et al., “Brixsino High-Flux Dual X-Ray and THz Radiation Source Based on Energy Recovery Linacs”, in Proc. 13th Int. Particle Accelerator Conf. (IPAC'22), Bangkok, Thailand, Jun. 2022, pp. 2407-2410.
D. Sertore et al., “Photocathode Stress Test Bench at INFN LASA”, in Proc. 13th Int. Particle Accelerator Conf. (IPAC'22), Bangkok, Thailand, Jun. 2022, pp. 2627-2629.
S. Samsam et al., “The HOMEN Model: An Estimator of High Order Modes Evolution in an Energy Recovery Linac”, in Proc. 13th Int. Particle Accelerator Conf. (IPAC'22), Bangkok, Thailand, Jun. 2022, pp. 2342-2345.
S. Samsam et al., “HOM Damping in Multi-Cell Superconducting Cavities for the Future Electron Source BriXSinO”, in Proc. 31st Linear Accelerator Conf. (LINAC'22), Liverpool, UK, Aug.-Sep. 2022, pp. 739-742.
C. Curatolo and L. Serafini, “A New Paradigm for Ultra-Low Emittance Muon Beam Generation Based on E.R.L.”, presented at the 31st Linear Accelerator Conf. (LINAC'22), Liverpool, UK, Aug.-Sep. 2022, paper WE1AA06, unpublished.
M. Rossetti Conti, A. Bacci, D. Giove, S. Samsam, L. Serafini, and D. Sertore, “Achromatic low energy merger for energy recovery linacs”, in Proc. 14th Int. Particle Accelerator Conf. (IPAC'23), Venice, Italy, May 2023, paper MOPA019, pp. 81-84.
S. Samsam et al., “High order mode analysis in energy recovery linac based on an energy budget model”, in Proc. 14th Int. Particle Accelerator Conf. (IPAC'23), Venice, Italy, May 2023, paper MOPA018, pp. 77-80.


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