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@ARTICLE{DArcy:459332,
      author       = {D'Arcy, Richard and Chappell, James and Beinortaite, Judita
                      and Diederichs, Severin and Boyle, Gregory James and Foster,
                      Brian and Garland, Matthew James and Gonzalez Caminal, Pau
                      and Lindstroem, Carl Andreas and Loisch, Gregor and
                      Schreiber, Siegfried and Schröder, Sarah and Shalloo, Rob
                      and Thévenet, Maxence and Wesch, Stephan and Wing, Matthew
                      and Osterhoff, Jens},
      title        = {{R}ecovery time of a plasma-wakefield accelerator},
      journal      = {Nature},
      volume       = {603},
      issn         = {0028-0836},
      address      = {London [u.a.]},
      publisher    = {Nature Publ. Group},
      reportid     = {PUBDB-2021-02538, arXiv:2203.01571. arXiv:2203.01571},
      pages        = {58 - 62},
      year         = {2022},
      note         = {Nature 603, 58-62 (2022)},
      abstract     = {The interaction of intense particle bunches with plasma can
                      give rise to plasma wakes capable of sustaining
                      gigavolt-per-metre electric fields, which are orders of
                      magnitude higher than provided by state-of-the-art
                      radio-frequency technology. Plasma wakefields can,
                      therefore, strongly accelerate charged particles and offer
                      the opportunity to reach higher particle energies with
                      smaller and hence more widely available accelerator
                      facilities. However, the luminosity and brilliance demands
                      of high-energy physics and photon science require particle
                      bunches to be accelerated at repetition rates of thousands
                      or even millions per second, which are orders of magnitude
                      higher than demonstrated with plasma-wakefield technology.
                      Here we investigate the upper limit on repetition rates of
                      beam-driven plasma accelerators by measuring the time it
                      takes for the plasma to recover to its initial state after
                      perturbation by a wakefield. The many-nanosecond-level
                      recovery time measured establishes the in-principle
                      attainability of megahertz rates of acceleration in plasmas.
                      The experimental signatures of the perturbation are well
                      described by simulations of a temporally evolving parabolic
                      ion channel, transferring energy from the collapsing wake to
                      the surrounding media. This result establishes that
                      plasma-wakefield modules could be developed as feasible
                      high-repetition-rate energy boosters at current and future
                      particle-physics and photon-science facilities.},
      keywords     = {accelerator: plasma (INSPIRE) / plasma: wake field
                      (INSPIRE) / acceleration (INSPIRE) / brightness (INSPIRE) /
                      charged particle: yield (INSPIRE) / performance (INSPIRE) /
                      accelerator: technology (INSPIRE)},
      cin          = {MPA2 / $HH_FH_FTX_AS$ / MPA1 / FTX / FS-PS / MIN / MFL},
      ddc          = {500},
      cid          = {I:(DE-H253)MPA2-20210408 /
                      $I:(DE-H253)HH_FH_FTX_AS-20210421$ /
                      I:(DE-H253)MPA1-20210408 / I:(DE-H253)FTX-20210408 /
                      I:(DE-H253)FS-PS-20131107 / I:(DE-H253)MIN-20120731 /
                      I:(DE-H253)MFL-20120731},
      pnm          = {621 - Accelerator Research and Development (POF4-621) / PWA
                      - Research group for plasma-based accelerators
                      (PWA-20150304) / 6G2 - FLASH (DESY) (POF4-6G2)},
      pid          = {G:(DE-HGF)POF4-621 / G:(DE-H253)PWA-20150304 /
                      G:(DE-HGF)POF4-6G2},
      experiment   = {EXP:(DE-H253)FLASHForward-20150101 /
                      EXP:(DE-H253)FLASH(machine)-20150101 /
                      EXP:(DE-H253)FLASHII(machine)-20150901},
      typ          = {PUB:(DE-HGF)16},
      eprint       = {2203.01571},
      howpublished = {arXiv:2203.01571},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:2203.01571;\%\%$},
      pubmed       = {pmid:35236975},
      UT           = {WOS:000763605400011},
      doi          = {10.1038/s41586-021-04348-8},
      url          = {https://bib-pubdb1.desy.de/record/459332},
}