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Terahertz-driven linear electron acceleration

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Miller,  R. J. Dwayne
Miller Group, Atomically Resolved Dynamics Department, Max Planck Institute for the Structure and Dynamics of Matter, Max Planck Society;
Center for Free-Electron Laser Science and The Hamburg Center for Ultrafast Imaging, Hamburg 22607, Germany;
Department of Chemistry and Physics, University of Toronto, Toronto, Ontario M5S, Canada;

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Citation

Nanni, E. A., Huang, W. R., Hong, K.-H., Ravi, K., Fallahi, A., Moriena, G., et al. (2015). Terahertz-driven linear electron acceleration. Nature Communications, 6: 8486. doi:10.1038/ncomms9486.


Cite as: https://hdl.handle.net/11858/00-001M-0000-0028-927E-C
Abstract
The cost, size and availability of electron accelerators are dominated by the achievable accelerating gradient. Conventional high-brightness radio-frequency accelerating structures operate with 30–50 MeV m−1 gradients. Electron accelerators driven with optical or infrared sources have demonstrated accelerating gradients orders of magnitude above that achievable with conventional radio-frequency structures. However, laser-driven wakefield accelerators require intense femtosecond sources and direct laser-driven accelerators suffer from low bunch charge, sub-micron tolerances and sub-femtosecond timing requirements due to the short wavelength of operation. Here we demonstrate linear acceleration of electrons with keV energy gain using optically generated terahertz pulses. Terahertz-driven accelerating structures enable high-gradient electron/proton accelerators with simple accelerating structures, high repetition rates and significant charge per bunch. These ultra-compact terahertz accelerators with extremely short electron bunches hold great potential to have a transformative impact for free electron lasers, linear colliders, ultrafast electron diffraction, X-ray science and medical therapy with X-rays and electron beams.