1990
DOI: 10.1017/s0263034600008041
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Picosecond high power KrF laser system for X-ray laser research

Abstract: Fundamental parameters are studied for the detailed design of a picosecond high power KrF laser system. The saturation energy density of 2.3 mJ/cm 2 and gain recovery time of 1.9 ns in an e-beam pumped KrF laser are observed. A 6 ps pulse is amplified to 1.9 J. The system at the Electrotechnical Laboratory is expected to deliver 10 ps pulses with total energy of several tens of joules in several beams.

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Cited by 7 publications
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“…The remaining values for the KrF medium's parameters assumed for determination of Es and the gain recovery curve are listed in Table I. 5 • 2, 2 ~r=3.7• and 3 [10]] and after measurement (points) from: (a) [50], (b) [57], (c) [58], (d) [59], (e) [60], (f) [61], and (g) [62] (2 ns pulse). 5 • 2, 2 ~r=3.7• and 3 [10]] and after measurement (points) from: (a) [50], (b) [57], (c) [58], (d) [59], (e) [60], (f) [61], and (g) [62] (2 ns pulse).…”
Section: Eout = Es Ln{1 + E X P ( G O L ) [ E X P ( E M / E S ) -11}mentioning
confidence: 99%
“…The remaining values for the KrF medium's parameters assumed for determination of Es and the gain recovery curve are listed in Table I. 5 • 2, 2 ~r=3.7• and 3 [10]] and after measurement (points) from: (a) [50], (b) [57], (c) [58], (d) [59], (e) [60], (f) [61], and (g) [62] (2 ns pulse). 5 • 2, 2 ~r=3.7• and 3 [10]] and after measurement (points) from: (a) [50], (b) [57], (c) [58], (d) [59], (e) [60], (f) [61], and (g) [62] (2 ns pulse).…”
Section: Eout = Es Ln{1 + E X P ( G O L ) [ E X P ( E M / E S ) -11}mentioning
confidence: 99%