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000275409 1001_ $$0P:(DE-HGF)0$$aNanni, Emilio A.$$b0$$eCorresponding author
000275409 245__ $$aTerahertz-driven linear electron acceleration
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000275409 520__ $$aThe 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 keVenergy  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.
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000275409 7001_ $$0P:(DE-HGF)0$$aHuang, Wenqian R.$$b1
000275409 7001_ $$0P:(DE-HGF)0$$aHong, Kyung-Han$$b2
000275409 7001_ $$0P:(DE-H253)PIP1019059$$aRavi, Koustuban$$b3
000275409 7001_ $$0P:(DE-H253)PIP1017124$$aFallahi, Arya$$b4$$udesy
000275409 7001_ $$0P:(DE-HGF)0$$aMoriena, Gustavo$$b5
000275409 7001_ $$0P:(DE-HGF)0$$aDwayne Miller, R. J.$$b6
000275409 7001_ $$0P:(DE-H253)PIP1013198$$aKaertner, Franz$$b7$$eCorresponding author$$udesy
000275409 773__ $$0PERI:(DE-600)2553671-0$$a10.1038/ncomms9486$$gVol. 6, p. 8486 -$$p8486$$tNature Communications$$v6$$x2041-1723$$y2015
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