2009
DOI: 10.1103/physrevstab.12.020702
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Laser pulse shaping for generating uniform three-dimensional ellipsoidal electron beams

Abstract: A scheme of generating a uniform ellipsoidal laser pulse for high-brightness photoinjectors is discussed. The scheme is based on the chromatic aberration of a dispersive lens. Fourier optics simulation reveals the interplay of group velocity delay and dispersion in the scheme, as well as diffractions. Particle tracking simulation shows that the beam generated by such a laser pulse approaches the performance of that by an ideal ellipsoidal laser pulse and represents a significant improvement from the traditiona… Show more

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Cited by 31 publications
(26 citation statements)
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“…The latter equation hints that the blow-out regime is generally unfavorable to emittance when operating with high-charge bunches produced in low-peak-field rf guns. For this reason, directly shaping the laser profile to follow an ellipsoidal distribution would be more effective when an improvement of the transverse emittance is desired [5,46] and for our range of bunch charges.…”
Section: Transverse Emittancementioning
confidence: 99%
“…The latter equation hints that the blow-out regime is generally unfavorable to emittance when operating with high-charge bunches produced in low-peak-field rf guns. For this reason, directly shaping the laser profile to follow an ellipsoidal distribution would be more effective when an improvement of the transverse emittance is desired [5,46] and for our range of bunch charges.…”
Section: Transverse Emittancementioning
confidence: 99%
“…The drive laser strikes the photocathode surface to emit electrons. The temporal and transverse shape of the laser pulse, together with the quantum efficiency (QE) of the photocathode surface, determines the temporal and transverse distribution of the electron beam upon emission, which has a significant impact on beam brightness and FEL performance [5][6][7][8][9][10]. The temporal distribution can be manipulated with techniques such as polarization based pulse stacking with birefringent crystals [11], acousto-optic modulators [12,13] or spatial modulators at a dispersion region [14].…”
Section: Introductionmentioning
confidence: 99%
“…• Illuminate the cathode with short laser pulse (duration < 100 fs), called pancake-like distribution, and use the longitudinal space charge driven expansion to create a nearly ideal uniformly filled ellipsoidal distribution [39,50,51]; • Illuminate the cathode with long (≈few ps) and skinny (<100 µm spot size) laser pulse, also called cigar-like, and use the transverse space charge to drive the beam expansion [52].…”
Section: Non Linearity In the Longitudinal Phase Space Distributionmentioning
confidence: 99%