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E-164. Presented by Patrick Muggli E-162 Collaboration :. F.-J. Decker, M. J. Hogan, R. Iverson, C. O’Connell, P. Raimondi, R.H. Siemann, D. Walz Stanford Linear Accelerator Center B. Blue, C. E. Clayton, C. Huang , C. Joshi, K. A. Marsh, W. B. Mori University of California, Los Angeles - PowerPoint PPT Presentation
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U C L AP. Muggli, SLAC-DoE, 04/10/03
E-164Presented by
Patrick Muggli
E-162 Collaboration:F.-J. Decker, M. J. Hogan, R. Iverson, C. O’Connell, P. Raimondi, R.H. Siemann, D. Walz
Stanford Linear Accelerator Center
B. Blue, C. E. Clayton, C. Huang, C. Joshi, K. A. Marsh, W. B. Mori
University of California, Los Angeles
T. Katsouleas, S. Lee, P. Muggli
University of Southern California
and E-164+X:+ C. Barnes, P. Emma, P. Krejcik, D. Johnson, W. Lu, E. Oz
U C L AP. Muggli, SLAC-DoE, 04/10/03
Work supported by USDoE #DE-FG03-92ER40745, DE-AC03-76SF00515, #DE-FG03-98DP00211, #DE-FG03-92ER40727, NSF #ECS-9632735, NSF #DMS-9722121.
OUTLINE
• Past year: -E-162, PWFA with long e-, e+ bunches: z≈700 µm
• Next year: -E-164 PWFA with short e- bunches: z≈100 µm
• 5+ years: -E-164 PWFA with ultra-short e- bunches: z≈20 µm-Long term ideas
U C L AP. Muggli, SLAC-DoE, 04/10/03
PLASMA WAKEFIELD EXPERIMENT@ SLAC
3 km e-/e+
LINACFinal Focus Test Beam
3 km for 50 GeV e- and e+ 1 m for 1 GeV?
U C L AP. Muggli, SLAC-DoE, 04/10/03
PLASMA WAKEFIELD (e-)
• Plasma wave/wake excited by a relativistic particle bunch
• Plasma e- expelled by space charge forces => energy loss, focusing (ion channel formation rc≈(nb/ne)1/2r)
• Plasma e- rush back on axis => energy gain
• Plasma Wakefield Accelerator (PWFA) = TransformerBooster for high energy accelerator
++++++++++++++ ++++++++++++++++
----- --- ----------------
---- -----------
-------- ------- -------------------- - -
-
---- - -- ---
------ -- -- ---- - - - - - --
---- - -- - - - --- --
- -- - - - - -
---- - ----
------
electron beam
+ + + + + + + + + + ++ + + + + + + + + + + + + + +
+ + + + + + + + + + + + + + ++ + + + + + + + + + + + + + +-
- --
--- --
Accelerating Decelerating (Ez)
+ + + + + + + + + + + + + + +
+ + + + + + + + + + + + + + +
Focusing (Er)Defocusing
• Linear scaling: Eacc 110(MeV / m)N 2 1010
z / 0.6mm 2 ≈ 1/z2
@ kpez≈√2
U C L AP. Muggli, SLAC-DoE, 04/10/03
• Optical Transition Radiation(OTR)
• CHERENKOV (aerogel)
- Spatial resolution ≈100 µm - Energy resolution ≈30 MeV- Time resolution: ≈1 ps
5 10 15 20 25 30 35 40 45 50
5
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y
x10 20 30 40 50 60
10
20
30
40
50
60
y
x
e-,e+
N=21010
z=0.6 mmE=28.5 GeV
IonizingLaser Pulse
(193 nm) Li Plasma
ne≈21014 cm-3
L≈1.4 m
CherenkovRadiator
Streak Camera(1ps resolution)
Bending MagnetX-Ray
Diagnostic
Optical TransitionRadiators Dump
∫Cdt
Quadrupoles
Imaging Spectrometer25 m
EXPERIMENTAL SET UP
IP0:
IP2:
E-157:
50 100 150 200 250 300
50
100
150
200
250
y,E
x10 20 30 40 50 60 70 80 90 100
20
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x
E-162:
- 1:1 imaging, spatial resolution <9 µm
U C L AP. Muggli, SLAC-DoE, 04/10/03
CHANNELING OF e-
OTR Images ≈1m downstream from plasma
• insensitive to ne at matching, stabilize hose instability• Channeling of the beam over 1.4 m or >12
2z2
K 2 2
3
2 0
K pe
2c ne 1/ 2
In an ion channel:
Envelope equation:
K 2 n
ee2
0m
e2c2
2
4
Beam-plasma matching:
• ne, matched =2.51014 cm-3
0
100
200
300
400
500
600
0 0.5 1 1.5 2
07250cwMatchedBetatron.graph
Plasma OFFPlasma ONEnvelope Equation Fit
x (
µm
)
Plasma Density (1014 cm-3)
=30 µm
N=4410-5 m-rad
=0.11 m=0
0
50
100
150
200
250
300
0 0.5 1 1.5 2
BetaronFitLongBeta.graph
Plasma OFFPlasma ONEnvelope
x (µ
m)
Plasma Density ( cm-3)
L=1.4 m
0=50 µm
N
=1210-5 m-rad
0=1.16 m
0=-0.5
Not matched
U C L AP. Muggli, SLAC-DoE, 04/10/03
DYNAMIC FOCUSING WITHIN e- BUNCH
-100
0
100
200
300
400
-15 -10 -5 0 5 10 15FocusingEnergySpread.graph
Relative Energy (MeV)Gaussian Bunch (a.u)Focusing Field (a.u.)
Rel
ativ
e E
nerg
y (M
eV)
(ps)
• Correlated Energy Spread
Space-Time Correlationafter Energy Dispersion
0
0.05
0.1
0.15
-10 -5 0 5 10
FocusingFieldvariation.graphFocusing FieldGaussian Bunch (a.u.)
Focu
sing
Fie
ld (
MV
/m)
(ps)
1 2 3"Blow-Out" • Channel Formation
Dynamic Focusing
Head
Head
U C L AP. Muggli, SLAC-DoE, 04/10/03
Density (x1014 cm-3)
Beam
Siz
e (
m)
= -3.5 = -2.8 = -2.1 = -1.4
= -0.7 = 0 = 0.7 = 1.4
= 2.1 = 2.8 = 3.5 = 4.2
= Blowout
= 4.2
= -3.5
= Head
= Middle
DYNAMIC FOCUSING WITHIN e- BUNCH
• Different t or z bunch slices experience a different number of betatron oscillations C. O’Connell et al., PRST-AB (2002)
U C L AP. Muggli, SLAC-DoE, 04/10/03
e-: ne0=21014 cm-3, c/p=375 µm e+: ne0=21012 cm-3, c/p=3750 µm
r=35 µmr=700 µm
• Uniformfocusing force (r,z)
=1.81010
• Non-uniformfocusing force (r,z)
d=2 mm
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
BlowOut
3 beamFront
Back
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
30 beamFront
Back
3-D QuickPIC simulations, plasma e- density:e- & e+ BEAM NEUTRALIZATION
e- e+
U C L AP. Muggli, SLAC-DoE, 04/10/03
0
200
400
600
800
1000
1200
1400
1600
0 1 2 3 4 5 6
122300cs-qdTriangxyNe.graph
x-Plasma OFFx-Plasma ONy-Plasma OFFy-Plasma ON
FW
HM
Tria
ngle
OT
R (
µm
)
ne (1014 cm-3)
FOCUSING OF e-/e+: HIGH ne
• from OTR images ≈1m from plasma exit
• Focusing limited by emittance growth due to plasma focusing aberrations?
0
50
100
150
200
250
300
0 0.5 1 1.5 2
BetaronFitLongBeta.graph
Plasma OFFPlasma ONEnvelope
x (µ
m)
Plasma Density ( cm-3)
L=1.4 m
0=50 µm
N
=1210-5 m-rad
0=1.16 m
0=-0.5
for e-:
M.J. Hogan et al., PRL (2003)
U C L AP. Muggli, SLAC-DoE, 04/10/03
FOCUSING OF e-/e+
0 50 100 150 200 250 300 350 400 450 500
50
100
150
200
250
300
0 50 100 150 200 250 300 350 400 450 500
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100
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300
0 50 100 150 200 250 300 350
50
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150
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30050 100 150 200 250 300 350
50
100
150
200
250
300
e-
e+
ne=0 ne≈1014 cm-3
2mm
2mm
• Ideal Plasma Lens in Blow-Out Regime
• Plasma Lens with Aberrations
• OTR images ≈1m from plasma exit (x≠y)
U C L AP. Muggli, SLAC-DoE, 04/10/03
EXPECTED ENERGY LOSS/GAIN, e-
• Expected energy gain < incoming correlated energy spread => need time discrimination
• Expected energy gain: 260 MeV (average), 335 MeV (peak)
• Expected energy loss: 95 MeV (average)
-200
-100
0
100
200
300
400
0
2
4
6
8
10
12
-8 -6 -4 -2 0 2 4 6 8SimualtionE(z).graph
(ps)
Front Back
Emax
Emin
Eav
2-D OSIRIS PIC simulation: L=1.4 m, ne=1.51014 cm-3, z=40 µm
-100
0
100
200
300
400
-15 -10 -5 0 5 10 15CorrelatedEnergy.graph
Relative Energy (MeV)Gaussian Bunch (a.u.)Longitudinal E-Field (a.u.)
Rel
ativ
e E
nerg
y (M
eV)
(ps)
Head
fp=110 GHz @ ne=1.51014 cm-3
U C L AP. Muggli, SLAC-DoE, 04/10/03
ENERGY GAIN/LOSS AVERAGE, e-
• Average energy gain (slice average): 156 ±40 MeV (≈3107 e-)• Average energy loss (slice average): 159±40 MeV
-200
-150
-100
-50
0
50
100
150
200
-6 -4 -2 0 2 4 6 8
SliceEnergyGain3curves.graph
ne=1.61014 (cm-3)
ne=2.01014 (cm-3)
ne=(2.3±0.1)1014 (cm-3)
Rel
ativ
e E
nerg
y (M
eV)
(ps)
+z
+2z
+3z
-2z
-z
ps slice analysis results
• Events/particles to more than 250 MeV
U C L AP. Muggli, SLAC-DoE, 04/10/03
Very Little Energy Spread
e+- beam:E 28.5 GeVN 1.21010 e+
z 0.73 mmr 40 µmrN 1210-5 m rad
Design Charge:21010
Ene
rgy
Spr
ead≈
1.5%
E
x
Low Charge: 1.21010
E
x
ENERGY LOSS/GAIN LOW CHARGE, e+
Cerenkov images => energy spectrum
• Lower charge allows for better time dispersed energy measurements
U C L AP. Muggli, SLAC-DoE, 04/10/03
ENERGY LOSS/GAIN LOW CHARGE e+
• Excellent agreement!
Plasma Off
Front Back
ne=1.81014cm-3
Loss Gain
Front Back
ne=1.81014cm-3
Experiment 2-D SimulationN=1.21010 e+
• Loss ≈ 50 MeV
• Gain ≈ 75 MeV
• Loss ≈ 45 MeV/m 1.4 m=63 MeV
• Gain ≈ 60 MeV/m 1.4 m=84 MeV
B. Blue et al., submitted to PRL
U C L AP. Muggli, SLAC-DoE, 04/10/03
0.01
0.1
1
10
100
1000
10 100 1000
E_useful [GV/m]
E_decel [GV/m]
E_spike [GV/m]
Ez [G
V/m
]
z [µm]
N = 1010
e-/bunch, r=10,20 µm
E-1
62E
-157
E-1
64
E-1
64X
NUMERICAL SIMULATIONS: E-164/X , e-
• E-164X: z=20-10 µm: >10 GV/m acceleration! (r dependent!)• Plasma length, energy gain limited by FFTB dump line acceptance
0.2 GV/m4.343106
fp=2.8 THz, W=3MT/m @ ne=1017 cm-3
U C L AP. Muggli, SLAC-DoE, 04/10/03
E-164: RIGHT NOW!
• Goal: >1 GeV over 30 cm (4 GeV/m)• Plasma length, energy gain limited by FFTB dump line acceptance
fp≈700 GHz, W=3MT/m @ ne=51015 cm-3
Beam tuning set up Lithium plasma source
OTRs at plasma entrance/exit UV-photo-ionized plasma
U C L AP. Muggli, SLAC-DoE, 04/10/03
E-164X: BEAM-IONIZED PLASMA
• Plasma source: neL limited by laser fluence and absorption
1010
1011
1012
1013
1014
1015
1016
1017
0 200 400 600 800 1000
VaporPressureLiCs.graph
Temperature (K)
Cesium Lithium
• Relativistic plasma electrons=> ne > given by kpz≈√2 ne≈1016-1017 cm-3
• Short bunch, Er≈5.210-19N/z r (GV/m) > tunneling field (Kyldish, ADK)
• Channeling+long plasma+large gradient=large energy gain!
N=1010 e-, z=r=20 µm in Cs
• Plasma density = neutral density (nf=1), easier, more stable!
Vapor pressure curves
U C L AP. Muggli, SLAC-DoE, 04/10/03
• Propagation in long field ionized plasmas, large energy gains
• Two-bunch experiments: - wake loading(ORION) - beam quality (, ∆E/E, ...)
• ... “Pre-After-Burner”
5+ YEARS
• Stability against hose the instability
U C L AP. Muggli, SLAC-DoE, 04/10/03
• Wealth of important results: - Beam refraction, Muggli et al., Nature 2001- Electrons transverse dynamics, Clayton et al., PRL 2002 - High brightness X-ray emission, Wang et al., PRL2002- Focusing dynamics, O’Connell et al., PRSTAB 2002- Positrons dynamic focusing, Hogan et al., PRL 2003- Acceleration of positrons, Blue et al., submitted to PRL - Acceleration of electrons, Muggli et al., in preparation
• E-157/162 built a PWFA laboratory for 30 GeV beams
• E-164: 1 GeV energy gain over 30 cm, PWFA z scaling law
• E-164X: Ultra short bunches, ultra-high gradients in field-ionized plasmas
SUMMARY
• Two-bunch experiments, hose instability, ultra-high energy gains, after-burner.