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Acceleration of electrons in the plasma wakefield of a proton bunch

Author

Listed:
  • E. Adli

    (University of Oslo)

  • A. Ahuja

    (CERN)

  • O. Apsimon

    (University of Manchester
    Cockcroft Institute)

  • R. Apsimon

    (Cockcroft Institute
    Lancaster University)

  • A.-M. Bachmann

    (CERN
    Max Planck Institute for Physics
    Technical University Munich)

  • D. Barrientos

    (CERN)

  • F. Batsch

    (CERN
    Max Planck Institute for Physics
    Technical University Munich)

  • J. Bauche

    (CERN)

  • V. K. Berglyd Olsen

    (University of Oslo)

  • M. Bernardini

    (CERN)

  • T. Bohl

    (CERN)

  • C. Bracco

    (CERN)

  • F. Braunmüller

    (Max Planck Institute for Physics)

  • G. Burt

    (Cockcroft Institute
    Lancaster University)

  • B. Buttenschön

    (Max Planck Institute for Plasma Physics)

  • A. Caldwell

    (Max Planck Institute for Physics)

  • M. Cascella

    (UCL)

  • J. Chappell

    (UCL)

  • E. Chevallay

    (CERN)

  • M. Chung

    (UNIST)

  • D. Cooke

    (UCL)

  • H. Damerau

    (CERN)

  • L. Deacon

    (UCL)

  • L. H. Deubner

    (Philipps-Universität Marburg)

  • A. Dexter

    (Cockcroft Institute
    Lancaster University)

  • S. Doebert

    (CERN)

  • J. Farmer

    (Heinrich-Heine-University of Düsseldorf)

  • V. N. Fedosseev

    (CERN)

  • R. Fiorito

    (Cockcroft Institute
    University of Liverpool)

  • R. A. Fonseca

    (ISCTE—Instituto Universitéario de Lisboa)

  • F. Friebel

    (CERN)

  • L. Garolfi

    (CERN)

  • S. Gessner

    (CERN)

  • I. Gorgisyan

    (CERN)

  • A. A. Gorn

    (Budker Institute of Nuclear Physics SB RAS
    Novosibirsk State University)

  • E. Granados

    (CERN)

  • O. Grulke

    (Max Planck Institute for Plasma Physics
    Technical University of Denmark)

  • E. Gschwendtner

    (CERN)

  • J. Hansen

    (CERN)

  • A. Helm

    (Universidade de Lisboa)

  • J. R. Henderson

    (Cockcroft Institute
    Lancaster University)

  • M. Hüther

    (Max Planck Institute for Physics)

  • M. Ibison

    (Cockcroft Institute
    University of Liverpool)

  • L. Jensen

    (CERN)

  • S. Jolly

    (UCL)

  • F. Keeble

    (UCL)

  • S.-Y. Kim

    (UNIST)

  • F. Kraus

    (Philipps-Universität Marburg)

  • Y. Li

    (University of Manchester
    Cockcroft Institute)

  • S. Liu

    (TRIUMF)

  • N. Lopes

    (Universidade de Lisboa)

  • K. V. Lotov

    (Budker Institute of Nuclear Physics SB RAS
    Novosibirsk State University)

  • L. Maricalva Brun

    (CERN)

  • M. Martyanov

    (Max Planck Institute for Physics)

  • S. Mazzoni

    (CERN)

  • D. Medina Godoy

    (CERN)

  • V. A. Minakov

    (Budker Institute of Nuclear Physics SB RAS
    Novosibirsk State University)

  • J. Mitchell

    (Cockcroft Institute
    Lancaster University)

  • J. C. Molendijk

    (CERN)

  • J. T. Moody

    (Max Planck Institute for Physics)

  • M. Moreira

    (CERN
    Universidade de Lisboa)

  • P. Muggli

    (CERN
    Max Planck Institute for Physics)

  • E. Öz

    (Max Planck Institute for Physics)

  • C. Pasquino

    (CERN)

  • A. Pardons

    (CERN)

  • F. Peña Asmus

    (Max Planck Institute for Physics
    Technical University Munich)

  • K. Pepitone

    (CERN)

  • A. Perera

    (Cockcroft Institute
    University of Liverpool)

  • A. Petrenko

    (CERN
    Budker Institute of Nuclear Physics SB RAS)

  • S. Pitman

    (Cockcroft Institute
    Lancaster University)

  • A. Pukhov

    (Heinrich-Heine-University of Düsseldorf)

  • S. Rey

    (CERN)

  • K. Rieger

    (Max Planck Institute for Physics)

  • H. Ruhl

    (Ludwig-Maximilians-Universität)

  • J. S. Schmidt

    (CERN)

  • I. A. Shalimova

    (Novosibirsk State University
    Institute of Computational Mathematics and Mathematical Geophysics SB RAS)

  • P. Sherwood

    (UCL)

  • L. O. Silva

    (Universidade de Lisboa)

  • L. Soby

    (CERN)

  • A. P. Sosedkin

    (Budker Institute of Nuclear Physics SB RAS
    Novosibirsk State University)

  • R. Speroni

    (CERN)

  • R. I. Spitsyn

    (Budker Institute of Nuclear Physics SB RAS
    Novosibirsk State University)

  • P. V. Tuev

    (Budker Institute of Nuclear Physics SB RAS
    Novosibirsk State University)

  • M. Turner

    (CERN)

  • F. Velotti

    (CERN)

  • L. Verra

    (CERN
    University of Milan)

  • V. A. Verzilov

    (TRIUMF)

  • J. Vieira

    (Universidade de Lisboa)

  • C. P. Welsch

    (Cockcroft Institute
    University of Liverpool)

  • B. Williamson

    (University of Manchester
    Cockcroft Institute)

  • M. Wing

    (UCL)

  • B. Woolley

    (CERN)

  • G. Xia

    (University of Manchester
    Cockcroft Institute)

Abstract

High-energy particle accelerators have been crucial in providing a deeper understanding of fundamental particles and the forces that govern their interactions. To increase the energy of the particles or to reduce the size of the accelerator, new acceleration schemes need to be developed. Plasma wakefield acceleration1–5, in which the electrons in a plasma are excited, leading to strong electric fields (so called ‘wakefields’), is one such promising acceleration technique. Experiments have shown that an intense laser pulse6–9 or electron bunch10,11 traversing a plasma can drive electric fields of tens of gigavolts per metre and above—well beyond those achieved in conventional radio-frequency accelerators (about 0.1 gigavolt per metre). However, the low stored energy of laser pulses and electron bunches means that multiple acceleration stages are needed to reach very high particle energies5,12. The use of proton bunches is compelling because they have the potential to drive wakefields and to accelerate electrons to high energy in a single acceleration stage13. Long, thin proton bunches can be used because they undergo a process called self-modulation14–16, a particle–plasma interaction that splits the bunch longitudinally into a series of high-density microbunches, which then act resonantly to create large wakefields. The Advanced Wakefield (AWAKE) experiment at CERN17–19 uses high-intensity proton bunches—in which each proton has an energy of 400 gigaelectronvolts, resulting in a total bunch energy of 19 kilojoules—to drive a wakefield in a ten-metre-long plasma. Electron bunches are then injected into this wakefield. Here we present measurements of electrons accelerated up to two gigaelectronvolts at the AWAKE experiment, in a demonstration of proton-driven plasma wakefield acceleration. Measurements were conducted under various plasma conditions and the acceleration was found to be consistent and reliable. The potential for this scheme to produce very high-energy electron bunches in a single accelerating stage20 means that our results are an important step towards the development of future high-energy particle accelerators21,22.

Suggested Citation

  • E. Adli & A. Ahuja & O. Apsimon & R. Apsimon & A.-M. Bachmann & D. Barrientos & F. Batsch & J. Bauche & V. K. Berglyd Olsen & M. Bernardini & T. Bohl & C. Bracco & F. Braunmüller & G. Burt & B. Butten, 2018. "Acceleration of electrons in the plasma wakefield of a proton bunch," Nature, Nature, vol. 561(7723), pages 363-367, September.
  • Handle: RePEc:nat:nature:v:561:y:2018:i:7723:d:10.1038_s41586-018-0485-4
    DOI: 10.1038/s41586-018-0485-4
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