2008
DOI: 10.1016/j.nima.2008.04.083
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Generation of ultra-short, high brightness electron beams for single-spike SASE FEL operation

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Cited by 92 publications
(51 citation statements)
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“…High brightness electron beam sources play a fundamental role in high-gain free-electron lasers (FEL) development as well as for linear colliders designed to study the electron-positron collisions [1,2]. For example, the SPARC project of INFN for generating 500 nm of wavelength has required laser-driven rf photocathode guns capable of producing 1 nC bunches of a few picosecond duration with about 1 mm-mrad of emittance [3,4].…”
Section: Introductionmentioning
confidence: 99%
“…High brightness electron beam sources play a fundamental role in high-gain free-electron lasers (FEL) development as well as for linear colliders designed to study the electron-positron collisions [1,2]. For example, the SPARC project of INFN for generating 500 nm of wavelength has required laser-driven rf photocathode guns capable of producing 1 nC bunches of a few picosecond duration with about 1 mm-mrad of emittance [3,4].…”
Section: Introductionmentioning
confidence: 99%
“…Several techniques have been explored to increase longitudinal coherence, stability, and/or to shorten the FEL pulse time scale towards the attosecond domain. The amplification of one single SASE spike has been demonstrated by compressing the electron beam close or below the FEL coherence length [15,16], by using a chirped bunch energy combined with a matched undulator taper [17][18][19], or by spoiling the whole electron beam except a limited fraction [20,21], a technique that has also been implemented to produce double pulse two-color radiation for pump and probe experiments [22]. Short single or multiple pulses have also been produced in seeded or cascaded FELs [23][24][25][26][27], with increased coherence and shot to shot stability.…”
mentioning
confidence: 99%
“…For instance, one may just reduce the beam charge to produce a very short electron bunch that naturally produces a very short FEL pulse [1][2][3] . Alternatively, one may use the so-called 'slotted foil' in the center of a chicane to spoil the transverse emittance for most of the portions of the electron beam such that an ultrashort x-ray pulse is produced only from the short slices of unspoiled beam that passes cleanly through the slot [4][5][6] .…”
Section: Introductionmentioning
confidence: 99%