The Seventh Workshop on Advanced Accelerator Concepts 1997
DOI: 10.1063/1.53051
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Summary report: Working group 7 on “laser sources for particle acceleration”

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Cited by 2 publications
(1 citation statement)
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“…(13), X-proportional increase in N. allows X2-proportional reduction in J Then, the average laser power calculated from Pm = P~T~f (14) scales as Pm -l/A. For example, to meet the extremely luminosity requirements for the IM.ue e-e+ collider, A= 1035s-lcm-2 [13], the picosecond C02 laser of the 10 kW average power may be required. The equivalent l-pm laser driver must be of the 100 kW power!…”
Section: Optimum Laser Driver For High Brightness Mono-energetic Lwfamentioning
confidence: 99%
“…(13), X-proportional increase in N. allows X2-proportional reduction in J Then, the average laser power calculated from Pm = P~T~f (14) scales as Pm -l/A. For example, to meet the extremely luminosity requirements for the IM.ue e-e+ collider, A= 1035s-lcm-2 [13], the picosecond C02 laser of the 10 kW average power may be required. The equivalent l-pm laser driver must be of the 100 kW power!…”
Section: Optimum Laser Driver For High Brightness Mono-energetic Lwfamentioning
confidence: 99%