Laser driver for a photocathode of an electron linear accelerator

A laser system is designed for operation with a photocathode electron gun for a linear accelerator with the following parameters of radiation at a wavelength of 262 nm (the fourth harmonic of a Nd:YLF laser). The pulse trains (macropulses) with a repetition rate of 5 Hz and a duration of 900 {mu}s c...

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Veröffentlicht in:Quantum electronics (Woodbury, N.Y.) N.Y.), 2011-01, Vol.40 (12), p.1123-1130
Hauptverfasser: Potemkin, A K, Gacheva, E I, Zelenogorskii, V V, Katin, E V, Kozhevatov, I E, Lozhkarev, V V, Luchinin, G A, Silin, D E, Khazanov, Efim A, Trubnikov, D V, Shirkov, G D, Kuriki, M, Urakava, J
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Sprache:eng
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Zusammenfassung:A laser system is designed for operation with a photocathode electron gun for a linear accelerator with the following parameters of radiation at a wavelength of 262 nm (the fourth harmonic of a Nd:YLF laser). The pulse trains (macropulses) with a repetition rate of 5 Hz and a duration of 900 {mu}s consist of 8-ps micropulses with an energy of 1.4 {mu}J and a repetition rate of 2.708 MHz. This repetition rate is variable within {+-}32 kHz and is stabilised by an external signal with an accuracy of 10 Hz. Due to the use of a feedback-controlled acousto-optic modulator, the root-mean-square deviation of the micropulse energy in the first and second harmonics is 2.5% and 3.6%, respectively. Using the decaying branch of the dependence of the second-to-fourth harmonic conversion efficiency on the second harmonic intensity, we decreased the root-mean-square deviation of the energy of the fourth-harmonic micropulses to 2.3% at the first-to-fourth harmonic conversion efficiency of 27%. (lasers and amplifiers)
ISSN:1063-7818
1468-4799
DOI:10.1070/QE2010v040n12ABEH014435