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Laser driven plasma wakefield accelerators and radiation sources · 2017. 9. 7. · ALPHA-X...

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ELI Bucharest 2011 ALPHA-X [email protected] Laser driven plasma wakefield accelerators and radiation sources Dino Jaroszynski University of Strathclyde
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  • ELI Bucharest 2011ALPHA-X [email protected]

    Laser driven plasma wakefield accelerators and radiation

    sources

    Dino JaroszynskiUniversity of Strathclyde

  • ELI Bucharest 2011ALPHA-X [email protected]

    Outline of talk• Large and small accelerators + high power lasers• Laser driven wakes• Ultra-short bunch electron production using wakefield

    accelerators • Betatron gamma ray source• Conclusion

  • ELI Bucharest 2011ALPHA-X [email protected]

    CERN – LHC27 km circumference

    SLAC

    50 GeV in 3.3 km

    20 MV/m

    7 TeV in 27 km

    7 MV/m

    Large accelerators depend on superconducting Radio Frequency cavities

  • ELI Bucharest 2011ALPHA-X [email protected]

    Synchrotrons light sources and free-electron lasers: tools for scientists

    Synchrotron – huge size and cost is determined by accelerator technology

    Diamond

    undulatorsynchrotron

    DESY undulator

  • ELI Bucharest 2011ALPHA-X [email protected]

    Particles accelerated by electrostatic fields of plasma waves

    Accelerators:

    Surf a 10’s cm long microwave –conventional technology

    Surf a 10’s mm long plasma wave –laser-plasma technology

    2

    max

    23

    gagg ª

    [V/cm]E e nª

  • ELI Bucharest 2011ALPHA-X [email protected]

    Wakefield acceleration

    lp

    Dephasing length: which gives a maximum energy:

    0g

    p

    wgw

    =

    204 3 ,d g pL c ag w=

    20

    23 g

    ag gª

  • ELI Bucharest 2011ALPHA-X [email protected]

    Bubble structure – relativistic regime

    laser

    self-injected electron bunch undergoing betatron oscillations

    ion bubble

    0

    2paR

    lªion bubble radius

  • ELI Bucharest 2011ALPHA-X [email protected]

    ALPHA-X started in 2002 Advanced Laser Plasma High-energy Accelerators towards X-rays

    Compact femtosecond duration particle, synchrotron, free-electron laser and gamma ray source l = 2.8 nm – 1 mm (

  • ELI Bucharest 2011ALPHA-X [email protected]

    ALPHA-X all-optical injection experiments on ASTRA

    800 nm

    350 – 540 mJ

    40 fs

    F/16 mirror

    gg ≈ 10

    1018 Wcm-2 in 25 mm spot

    a0 ~ 0.7 – 1

    ne~ 1.5 x 1019cm-3

    S. Mangles et al. Nature 2004

    3%dgg

    ª

    ALPHA-X: Imperial/RAL/Strathclyde

    t ~ 5 – 10 fsI ~ 5 kA

    Few fs duration electron bunch

    20

    max

    2150

    3gagg = ª

  • ELI Bucharest 2011ALPHA-X [email protected]

    LBNL - Oxford campaign (ALPHA-X) team: GeV beams from capillary

    Pre-formed plasma channels –Spence & Hooker (PRE 2001)

    W. Leemans, … S. Hooker, (Nature Physics 2006)

    ALPHA-X: Oxford & Berkeley

    Channels manufactured using laser machining techniques – Jaroszynski et al., (Royal Society Transactions, 2006)

  • ELI Bucharest 2011ALPHA-X [email protected]

    1 GeV beams

    50 pC 30 pC

    Acceleration to 1 GeV in 33 mm long pre-formed plasma channels

    5% shot-to-shot fluctuations in mean energy

    W. Leemans, … S.Hooker, (Nature Physics 2006)

    E = 0.48 GeV±6% and an r.m.s. spread

  • ELI Bucharest 2011ALPHA-X [email protected]

    210

    BENDINGMAGNET

    UNDULATOR

    ELECTRON ENERGYSPECTROMETER

    LASER IN

    PLASMA ACCELERATOR

    RADIATIONSPECTROMETER

    Strathclyde: ALPHA-X beam line

    8 m

    TOPS laser:1.1 J @ 10 Hzl = 800 nm30 fs

    Jaroszynski et al., (Royal Society Transactions, 2006)

  • ELI Bucharest 2011ALPHA-X [email protected]

    Experimental Results – energy stability

    Electron Spectrometer: 200 consecutive shots (spectrum on 196 shots)

    69 90 124 185Energy (MeV)

    100 consecutive shotsMean E0 = (137 ± 4) MeV

    2.8% stability

  • ELI Bucharest 2011ALPHA-X [email protected]

    Energy spread at 130 MeV

    100 110 120 130 140 150

    8000

    10000

    12000

    14000

    16000

    18000

    Char

    ge/u

    nit e

    nerg

    y [a

    .u.]

    Energy [MeV]

    0.75%gsg

    =

    63 MeV 170 MeV

    130 135 140 145 1500

    5

    10

    15

    20

    25

    30

    Coun

    ts

    Energy [MeV]

    r.m.s. spread of mean energy 2.8%

  • ELI Bucharest 2011ALPHA-X [email protected]

    -0.75 -0.50 -0.25 0.00 0.25 0.50 0.75

    -3

    -2

    -1

    0

    1

    2

    3

    4

    x' [m

    rad]

    x[mm]

    Experimental Results – emittance

    • divergence 1 – 2 mrad for this runwith 125 MeV electrons

    • average eN = (2.2 ± 0.7)p mm mrad• best eN = (1.0 ± 0.1)p mm mrad• Elliptical beam: eN, X > eN, Y

    • Second generation mask with hole f ~ 25 mm and improved detection system

    0 1 2 30

    5

    10

    Coun

    t

    enx [p mm mrad]

    (a)

    0 1 2 30

    5

    10

    Coun

    t

    eny [p mm mrad]

    (b)

  • ELI Bucharest 2011ALPHA-X [email protected]

    Ultra-short pulseMeasurements at Strathclyde indicate 1-2 fs electron bunches with

    1-10 pC: i.e. Multi kA peak current, with energy spread and emittance – suitable for FEL

  • ELI Bucharest 2011ALPHA-X [email protected]

    Synchrotron radiation from an ion channel wiggler: betatron radiation

    • Wiggler motion – electron deflection angle q ~(px/pz) is much larger than the angular spread of the radiation j=(1/γ)

    • Only when k & p point in the same direction do we get a radiation contribution.

    • Spectrum rich in harmonics – peaking at• Radiation rate therefore only emission at dephasing length

    1uag >> >>

    deflection angle – au /g

    j=1/g

    338

    ucrit

    ah ª2W gµ dL

  • ELI Bucharest 2011ALPHA-X [email protected]

    SCALING LAWS

    • Betatron Frequency: • Transverse momentum:• Divergence: • Critical photon Energy:• Efficiency:

    • Wavelength:

    / 2pbw w g=

    ea n rb bgµ

    /abJ g=2

    c eE n rbgµ

    Betatron radiation emission during LWFA

    /phot cycleN aba=

    2 22 2

    2 3/231 ( ) 1 ( )

    2 2 2h e ee p e

    a ach h

    b b bl pl g j g jg w g

    Ê ˆ Ê ˆ= + + = + +Á ˜ Á ˜

    Ë ¯ Ë ¯

  • ELI Bucharest 2011ALPHA-X [email protected]

    Gamma Ray Source demoistrated on Gemini using PW laser108 photons between .1 and 7 MeVBrilliance 1023 photons/(s mrad2 mm2 0.1%bandwidth) is

    femtosecond duration pulses

  • ELI Bucharest 2011ALPHA-X [email protected]

    Typical high energy spectra: Gemini experiment using plasma channel 85% of shots

  • ELI Bucharest 2011ALPHA-X [email protected]

    Synchrotron, betatron and FEL radiation peak brilliance

    ALPHA-X ideal 1GeV bunch

    FEL: Brilliance 5 – 7 orders of magnitude larger

    lu = 1.5 cm

    en = 1 p mm mrad

    te = 10 fs

    Q = 100 – 200 pC

    I = 25 kA

    dg/g < 1%

    I(k) ~ I0(k)(N+N(N-1)f(k)) FEL = spontaneous emission x 107

    betatron source

  • ELI Bucharest 2011ALPHA-X [email protected]

    The Scottish Centre for the Application of Plasma Based Accelerators: SCAPA

    1000 m2 laboratory space: 200-300 TW laser and 10 “beam lines” producing particles and radiation sources for applications: nuclear physics, health sciences, plasma physics, homeland security etc.

    New £100m Strathclyde Technology Innovation Centre

  • ELI Bucharest 2011ALPHA-X [email protected]

    Strathclyde (students and staff):Team: Dino Jaroszynski, Salima Abu-Azoum, Maria-Pia Anania, ConstantinAniculaesei, Rodolfo Bonifacio, Enrico Brunetti, Sijia Chen, Silvia Cipiccia, David Clark, Bernhard Ersfeld, John Farmer, David Grant, Ranaul Islam, Riju Issac, Yevgen Kravets, Tom McCanny, Grace Manahan, Adam Noble, Guarav Raj, Richard Shanks, Anna Subiel, Xue Yang, Gregory Vieux, Gregor Welsh and Mark WigginsCollaborators: Gordon Rob, Brian McNeil, Ken Ledingham and Paul McKenna

    ALPHA-X: Current and past collaborators:ELI-NP Bucharest, Lancaster U., Cockcroft Institute / STFC - ASTeC, STFC – RAL CLF, U. St. Andrews, U. Dundee, U. Abertay-Dundee, U. Glasgow, Imperial College, IST Lisbon, U. Paris-Sud - LPGP, Pulsar Physics, UTA, CAS Beijing, LBNL, FSU Jena, U. Stellenbosch, U. Oxford, LAL, U. Twente, TUE, U. Bochum, ....

    ALPHA-X project

    Current Support:

    EPSRC, E.U. Laserlab, STFC

    consortium

  • ELI Bucharest 2011ALPHA-X [email protected]

    FIN

    Thank you

    Laser driven plasma wakefield accelerators and radiation sources��Outline of talkCERN – LHC�27 km circumferenceSynchrotrons light sources and free-electron lasers: tools for scientistsParticles accelerated by electrostatic fields of plasma wavesWakefield accelerationBubble structure – relativistic regimeALPHA-X started in 2002 �Advanced Laser Plasma High-energy �Accelerators towards X-raysALPHA-X all-optical injection experiments on ASTRALBNL - Oxford campaign (ALPHA-X) team: GeV beams from capillary1 GeV beamsSlide Number 12Slide Number 13Energy spread at 130 MeVSlide Number 15Ultra-short pulseSlide Number 18Slide Number 19Gamma Ray Source demoistrated on Gemini using PW laserTypical high energy spectra: Gemini experiment using plasma channel 85% of shotsSynchrotron, betatron and FEL radiation peak brillianceThe Scottish Centre for the Application of Plasma Based Accelerators: SCAPASlide Number 26FIN��Thank you


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