Abstract
The scope of that contribution is to present the challenges of the next particle sources for accelerators. It is admitted1 that emittance near Interaction Point (IP) is strongly dominated by the emittance of the low power source. To minimize the Bremstrahlung effects in the Interaction Point (IP), we also need extremely low emittance bunches, ultra high brillance, very low charges sub fC, near depopulated attosecond electronic bunches. These produced bunches should fit the entrances of Dielectric Laser Accelerators (DLA) and Laser Plasma Accelerators (LPA).
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