2014
DOI: 10.1016/j.nima.2013.10.078
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Dielectric laser acceleration of 28keV electrons with the inverse Smith–Purcell effect

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Cited by 12 publications
(6 citation statements)
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“…These record gradients are enabled especially by modern ultrashort-pulsed laser systems, mostly in the infrared spectrum, and by challenging nanofabrication techniques for the high damage threshold dielectric materials, as adopted from the semiconductor industry. Due to these high technical demands, the experimental demonstration of electron acceleration in DLA came only in 2013, more than 50 years later than the original proposal [4,5]. These promising results of gradients, generating only energy spread till then , lead to the funding of the ACHIP collaboration [6] in 2015 , in order to achieve an accelerator on a chip attaining MeV energy gain.…”
Section: Introductionmentioning
confidence: 99%
“…These record gradients are enabled especially by modern ultrashort-pulsed laser systems, mostly in the infrared spectrum, and by challenging nanofabrication techniques for the high damage threshold dielectric materials, as adopted from the semiconductor industry. Due to these high technical demands, the experimental demonstration of electron acceleration in DLA came only in 2013, more than 50 years later than the original proposal [4,5]. These promising results of gradients, generating only energy spread till then , lead to the funding of the ACHIP collaboration [6] in 2015 , in order to achieve an accelerator on a chip attaining MeV energy gain.…”
Section: Introductionmentioning
confidence: 99%
“…structures are used to accelerate and manipulate particles via the inverse Smith-Purcell effect (hereinafter referred to as inverse Smith-Purcell (ISP-DLA)) [5][6][7][8][9][10]. Recently, a kind of DLA using the inverse Cherenkov effect (hereinafter referred to as inverse Cherenkov radiation (ICR-DLA)) has aroused great interest.…”
Section: Introductionmentioning
confidence: 99%
“…These record gradients are enabled especially by modern ultrashort-pulsed laser systems, mostly in the infrared spectrum, and by nanofabrication techniques for the high damage threshold dielectric materials, as adopted from the semiconductor industry. Due to these high technical demands, the experimental demonstration of electron acceleration in DLA came only in 2013, more than 50 years later than the original proposal [4,5]. These promising results of gradients, generating only energy spread so far, lead to the funding of the ACHIP collaboration [6], in order to achieve an accelerator attaining MeV energy gain.…”
Section: Introductionmentioning
confidence: 99%