High-intensity Lasers - fz-juelich.decollaborations.fz-juelich.de/ikp/cgswhp/cgswhp12/... · August...
Transcript of High-intensity Lasers - fz-juelich.decollaborations.fz-juelich.de/ikp/cgswhp/cgswhp12/... · August...
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August 9th, 2012 |
Mit
glie
d d
er
Helm
holt
z-G
em
ein
sch
aft
Ilhan Engin - IKP [email protected]
High-intensity Lasers
for particle physics
5th Georgian - German School and Workshop in Basic Science
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August 9th, 2012 Slide [email protected]
Working group
• Institute for Nuclear Physics (FZJ) M. Büscher *)
• Jülich Supercomputing Centre (FZJ) P. Gibbon *)
• Zentralinstitut für Technologie ZAT (FZJ) H. Soltner
• Institute for Laser and Plasma Physics, Heinrich Heine University Düsseldorf (HHUD) Prof. O. Willi *)
• Institute for Nuclear Physics,University of Münster (WWUM) Prof. A. Khoukaz *)
• in cooperation with RWTH Aachen University, University ofCologne
*) group leaders
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August 9th, 2012 Slide [email protected]
Outline
• Laser: New Generation of Particle Accelerators
• Polarized Beams
• Current Experiments at HHUD
S
Nµ
s
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August 9th, 2012 Slide [email protected]
Development of conventional accelerators and plasma driven particle sources
N. Raab, PhD thesis 2011
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August 9th, 2012 Slide [email protected]
Development of Laser intensities
Ch
ara
cter
istic
ele
ctro
n e
ne
rgy
Fo
cuss
ed in
ten
sity
I in
W/c
m²
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August 9th, 2012 Slide [email protected]
1367 W / m²
10 20 W / cm ²
Current Laser intensities
high-intense Lasers
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August 9th, 2012 Slide [email protected]
Düsseldorf ARCturus Laser facility
PULSAR Ti:Sapphire Laser: 100 TW, 800 nm~ 2.5 Joule, less than 25 femtoseconds
focused on 10 micronsInstitute for Laser and Plasma PhysicsProf. O.Willi - HHUD
chambers forgas target foil target
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August 9th, 2012 Slide [email protected]
Laser-induced particle acceleration
ultra-shorthigh-intenseLaser pulse
mass limited
target
gas jets
underdense plasma
solid targets
overdense plasma
new approach:
cluster jets
future plans:
H2 pellets
chargedparticles
electrons~ 100 MeV
protons / ions~ 10 MeV
*) typical values at HHUD
*)
*)
*)
I ~ 1020 W/cm2
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August 9th, 2012 Slide [email protected]
wake fieldoscillating electrons
laser pulse
plasma
Wake fields / bubbles
ponderomotive force
some electrons expel out of regions with higher intensity
some electrons oscillate
Laser-induced acceleration mechanisms
F pon ∝ −∇ I
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August 9th, 2012 Slide [email protected]
• lower intensities: wake fields
• high intensities: wake fields & bubble regime
A.Pukhov & J.Meyer-ter-Vehn, Appl. Phys. B 74, 355–361 (2002)
V.Malka et al., Nature Physics 4, 447–452 (2008)
ne/n
0
acceleration of electrons
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August 9th, 2012 Slide [email protected]
Target Normal Sheath Acceleration TNSA
proton acceleration from surface of thin foils (solid targets)
target foil
E ~ 100 GV/m
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August 9th, 2012 Slide [email protected]
Conventional vs. Laser-induced acceleration
100 µm100 GV/m
1 m1 MV/m } 1 MeV } 10 MeV
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August 9th, 2012 Slide [email protected]
Outline
• Laser: New Generation of Particle Accelerators
• Polarized Beams
• Current Experiments at HHUD
S
Nµ
s
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August 9th, 2012 Slide [email protected]
Spin-polarization (spin ≠ 0, e.g. protons)
• 1 particle spin
• Ensemble of particles
random spin-orientationhere: disordered spins
P = 0% = 0no polarization
all spins ordered in same directionhere: P = 100% = 1polarized particle beam
polarization
P =
N = occupation number of u/d - state
N up−N down
N upN down
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August 9th, 2012 Slide [email protected]
Strong electro-magnetic fields (simulation)
Simulations: A.Karmakar, P.Gibbon (IAS, FZJ)
5 · 1020 W/cm²λ = 0.81 µm; focus Ø = 5 µmduration: 30 fs; p-polarizedIncidence angle: 45°
5 · 1020 W/cm²λ = 0.81 µm; focus Ø = 5 µmduration: 30 fs; p-polarizedIncidence angle: 45°
B - field distribution 140 fs after laser hits target
field strength / gradient: ~ 104 T / 1010 T/m
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August 9th, 2012 Slide [email protected]
foil targets
gases / gas mixtures
( H2 He 3He )
cluster jets
polarized3He gas
2 possible scenarios for creating polarized particle beams
• Polarization is generated
Laser-acceleration process polarizes
particles from unpolarized targets (plasmas)
due to large magnetic fields and / or gradients
• Polarization is conserved
Spin direction is invariant in
strong laser & plasma fields
Polarized beams from Laser plasmas
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August 9th, 2012 Slide [email protected]
Scattering of a polarized particle beam
Observables, e.g.
diff. cross section
beam polarization P
analyzing power A
if P > 0 %
NLEFT ≠ NRIGHT
polarized particle beam
ϑ1
detector LEFT
detector RIGHT
ϑ2
dσ
dΩ(E ,ϑ)
point of interaction
(scattering target)
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August 9th, 2012 Slide [email protected]
beam polarization
P
-1 ≤ P ≤ 1
analyzing power
A ( E , ϑ , target )
-1 ≤ A ≤ 1
simplest case: particle (spin-½) on unpolarized particle
dσdΩ pol
(E ,ϑ ,φ) = dσdΩ unpol
(E ,ϑ) [1+A⋅P⋅cos(φ)]
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August 9th, 2012 Slide [email protected]
P = 0 or A = 0symmetric distribution
P = 1, A = 1asymmetric distribution
dσ
dΩ pol(E ,ϑ ,φ) = d σ
d Ωunpol(E ,ϑ) [1+A⋅P⋅cos(φ)]
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August 9th, 2012 Slide [email protected]
Outline
• Laser: New Generation of Particle Accelerators
• Polarized Beams
• Current Experiments at HHUD
S
Nµ
s
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August 9th, 2012 Slide [email protected]
Polarization measurement: setup
Ø = 1mm
Ep = 3.0 – 3.4 MeV
RCF stack
AnalyzingTarget
Si, d = 24 µm
analyzing power
A
known
Laser pulse1.2 J, 40 fs
Production Target
gold, d = 3 µm
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August 9th, 2012 Slide [email protected]
CR-39 plates
dσdϑ
A·P
Secondary scattering targetSi, d = 24 µm
Production target:gold, d = 3 µm
Laser pulse: 1.2 J, 40 fsincidence angle: 45°
Rate monitor:radiochromic film
5 cm
Detection of scatteredprotons:
CR-39 plates
Appertures Ø = 1mmfor angular selection
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August 9th, 2012 Slide [email protected]
Scattering-angle distribution
*) average over 10 shots
preli
mina
ry
Si(p, p’)Si, Tp = (3.2±0.2) MeV
(1994)
(2011)
Cologne Tandem ARCturus Laser
beam time ~ days beam time ~ 100 fs *)
N.Raab, Ph.D. thesis 2011
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August 9th, 2012 Slide [email protected]
Angular distribution of the proton polarization
φ
Laser incidence angle: φ = 90°, ϑ = 45°
Proton emission angle:φ = 180°, ϑ = 8°
Relative to production target normal
FitScattering angle ϑ = 50°
φ
dσ
dΩ (E ,ϑ ,φ) ∝ [1+A⋅P⋅cos(φ−φ0)]
P ≈ 0.08 ± 0.08stat,2σ ± 0.08systAveraging scattering angleϑ = 37.5° 57.5°̶
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August 9th, 2012 Slide [email protected]
Gas target experiments: H
2 4He 3He
pol-unpol H
2 clusters
gas target chamber
Laser beam
accelerated protons / ions
Supersonic gas jet
out of nozzle
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August 9th, 2012 Slide [email protected]
H2 cluster source
A. Täschner, http://arxiv.org/abs/1108.2653
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August 9th, 2012 Slide [email protected]
Outlook
• fundamental research
• comprehension of Laser-acceleration mechanisms
• advantages of Laser-accelerated high-energy particles
• possible applicability, e.g. in future accelerator physics,
synchrotron radiaton, etc.
• integration in existing or planned infrastructure, e.g. the planned
Ju-SPARC *) at FZJ
*) Short-Pulsed Particle and Radiation Center
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August 9th, 2012 Slide [email protected]