2017
DOI: 10.1063/1.4975892
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Structured electron beams from nano-engineered cathodes

Abstract: Abstract. The ability to engineer cathodes at the nano-scale have opened new possibilities such as enhancing quantum efficiency via surface-plasmon excitation, forming ultra-low-emittance beams, or producing structured electron beams. In this paper, we present numerical investigations of the beam dynamics associated with this class of cathode in the weak-and strong-field regimes. We finally discuss the possible applications of some of the achievable cathode patterns when coupled with other phase space manipula… Show more

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“…One promising application of the technique is the possible generation of narrowband electromagnetic radiation enhanced at the wavelength λ n ∼ ∆ζ/n (where n is an integer). Reaching ultrashort wavelength (high harmonic number n) will require the use of smaller laser pattern or nano-engineered cathodes capable of producing transversely-segmented beams 1,24,25 . In addition, attaining these finer-scale modulations will also require a thorough control of optical aberrations along the accelerator and in particular within the TLEX beamline 21,26 .…”
Section: Discussionmentioning
confidence: 99%
“…One promising application of the technique is the possible generation of narrowband electromagnetic radiation enhanced at the wavelength λ n ∼ ∆ζ/n (where n is an integer). Reaching ultrashort wavelength (high harmonic number n) will require the use of smaller laser pattern or nano-engineered cathodes capable of producing transversely-segmented beams 1,24,25 . In addition, attaining these finer-scale modulations will also require a thorough control of optical aberrations along the accelerator and in particular within the TLEX beamline 21,26 .…”
Section: Discussionmentioning
confidence: 99%
“…This new distribution is then used as a starting distribution in an RF gun and the corresponding dynamics simulated with the fast PIC program Astra [9]. To date our efforts have focused on transversely imaging the cathode-array structure downstream of an accelerator beamline with 4 × 4 transfer matrix R. Given the Courant-Snyder parameters [for the horizontal plane (α x,1 , β x,1 )] associated to a single beamlet (formed from a nanohole) along with the parameters computed of the entire beam (α x , β x ) we found a general relationship that ensure single-particle imaging in the horizontal plane to be [10] single-beamlet emittance [11]. The latter set of equations respectively force (i) each beamlet to be at a waist (we assume all the beamlets have identical parameters) and (ii) the entire beam to be collimated.…”
Section: Acceleration In An Rf Gunmentioning
confidence: 97%