1982
DOI: 10.1016/0167-5087(82)90291-5
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A study of a transverse optical klystron experiment in adone (TOKA)

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Cited by 23 publications
(11 citation statements)
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“…This is because the effective energy spread of finite emittace in the dispersion section is negligible. A detailed analysis has been given by Boscolo and Stagno [27]. The main result is rather simple, as explained in the following.…”
Section: B4 the Effect Of Finite Emittance In The Dispersion Sectionmentioning
confidence: 75%
“…This is because the effective energy spread of finite emittace in the dispersion section is negligible. A detailed analysis has been given by Boscolo and Stagno [27]. The main result is rather simple, as explained in the following.…”
Section: B4 the Effect Of Finite Emittance In The Dispersion Sectionmentioning
confidence: 75%
“…Assuming, just for an evaluation, an undulator of parameter K=1, which, consequently, would give a 27 cm long period and a number of periods N=10, the coherent spontaneous power in the first harmonic calculated following ref. [17] is Here η 0 is the free space impedance, I the electron beam current and A 1 the amplitude of the first harmonic bunching. Incidentally, this coherent power is a factor two less than that evaluated with the formula reported in the Handbook of Accelerator Physics and Engineering [18].…”
Section: Discussionmentioning
confidence: 99%
“…The generation of harmonics by bunching an electron beam in a wiggler, using a seed laser, is well known and verified experimentally [1]. The use of prebunching in FELs was studied analytically [2] and more recently, in a 3-D numerical simulation [3]. The extension of this technique to the exponential growth regime including wiggler tapering has been proposed and studied in detail as the basis for the UV-FEL User's Facility at BNL [4] [5] [6].…”
Section: Introductionmentioning
confidence: 97%