4.8 Article

Generation and acceleration of electron bunches from a plasma photocathode

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NATURE PHYSICS
卷 15, 期 11, 页码 1156-+

出版社

NATURE PUBLISHING GROUP
DOI: 10.1038/s41567-019-0610-9

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资金

  1. UCLA (US Department of Energy (DOE)) [DE-SC0009914]
  2. RadiaBeam Technologies (DOE) [DE-SC0009533]
  3. FACET E200 team
  4. DOE [DE-SC0011617, DE-AC02-76SF00515, DE-AC02-05CH11231]
  5. H2020 EuPRAXIA [653782]
  6. EPSRC [EP/N028694/1]
  7. Research Council of Norway [230450]
  8. US NSF [PHY-1734319]
  9. DFG Emmy-Noether programme
  10. JURECA [hhh36]
  11. HLRN
  12. US DOE Office of High Energy Physics [DE-SC0013855]
  13. National Science Foundation [PHY 1734281]
  14. [k1191]
  15. [VH-VI-503]
  16. U.S. Department of Energy (DOE) [DE-SC0013855, DE-SC0009914, DE-SC0009533] Funding Source: U.S. Department of Energy (DOE)
  17. EPSRC [1823175] Funding Source: UKRI
  18. STFC [ST/P002056/1] Funding Source: UKRI
  19. Engineering and Physical Sciences Research Council [1823175] Funding Source: researchfish

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Plasma waves generated in the wake of intense, relativistic laser(1,2) or particle beams(3,4) can accelerate electron bunches to gigaelectronvolt energies in centimetre-scale distances. This allows the realization of compact accelerators with emerging applications ranging from modern light sources such as the free-electron laser to energy frontier lepton colliders. In a plasma wakefield accelerator, such multi-gigavolt-per-metre wakefields can accelerate witness electron bunches that are either externally injected(5,6) or captured from the background plasma(7,8). Here we demonstrate optically triggered injection(9-11) and acceleration of electron bunches, generated in a multi-component hydrogen and helium plasma employing a spatially aligned and synchronized laser pulse. This 'plasma photocathode' decouples injection from wake excitation by liberating tunnel-ionized helium electrons directly inside the plasma cavity, where these cold electrons are then rapidly boosted to relativistic velocities. The injection regime can be accessed via optical(11) density down-ramp injection(12-16) and is an important step towards the generation of electron beams with unprecedented low transverse emittance, high current and 6D-brightness(17). This experimental path opens numerous prospects for transformative plasma wakefield accelerator applications based on ultrahigh-brightness beams.

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