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