simulation of the e+ source up to the clic damping ring
DESCRIPTION
Simulation of the e+ Source up to the CLIC Damping Ring. A. VIVOLI* Thanks to: L. RINOLFI (CERN) R. CHEHAB (IPNL & LAL / IN2P3-CNRS) O. DADOUN, F. POIRIER, P. LEPERCQ, A. VARIOLA (LAL / IN2P3-CNRS) V. STRAKHOVENKO (BINP) K. FLÖTTMANN (DESY). * E-mail : [email protected]. - PowerPoint PPT PresentationTRANSCRIPT
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Simulation of the e+ Source up to the CLIC Damping Ring
A. VIVOLI*
Thanks to:
L. RINOLFI (CERN)
R. CHEHAB (IPNL & LAL / IN2P3-CNRS)
O. DADOUN, F. POIRIER, P. LEPERCQ, A. VARIOLA (LAL / IN2P3-CNRS)
V. STRAKHOVENKO (BINP)
K. FLÖTTMANN (DESY)
* E-mail : [email protected]
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20/04/23A. Vivoli, CLIC Positron Source,
CLIC 2009, CERN2
CONTENTS
• General scheme of the CLIC positron source
• Design and Simulation of the elements
• Conclusions
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e- gun
LaserDC gunPolarized e-
Pre-injector Linac for e-
200 MeV
e-/Target
Pre-injector Linac for e+
200 MeV
Primary beam Linac for e-
5 GeV
Inje
ctor
Lin
ac
2.66
GeV
e+ DR
e+ PDRB
oost
er L
inac
5.
14 G
eV
4 GHz
e+ BC1 e- BC1
e+ BC2 e- BC2e+ Main Linac e- Main Linac
2 GHz
e- DR
e- PDR
2 GHz 2 GHz 2 GHz
4 GHz 4 GHz
12 GHz 12 GHz
8 GeV48 km
2.86 GeV 2.86 GeV
e
Target
AMD
2.86 GeV 2.86 GeV
3 TeV
Base line configuration
CLIC Main Beam Injector Complex (2009)
IP
Unpolarized e+
3
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4
POSITRON SOURCES USING CHANNELING FOR ILC & CLIC
• PROPOSED POSITRON TARGET FOR CLIC
e-
Crystal Amorphous
e+, e-, e-
e+
2 m
(5 GeV)
W: 1.4 mm thick W: 10 mm thick
N. simulated e- : 6000 r=2.5 mm
20/04/23 A. Vivoli, CLIC Positron Source, CLIC 2009, CERN
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Gamma Production
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PHOTONS SPECTRUM
CHANNELING: N = 111942 N / Ne- = 18.657 E = 170.37 MeV Ee- = 5 GeV
r = 9.85 mm
SPOT SIZE
By V. STRAKHOVENKO
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Positron Production
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N. e+ Yield e+/e-
x (rms)
mm mrad
y (rms)
mm mrad
<E> MeV
E
MeV
z (rms)* mm
49500 8.25 63614 77903 54.51 115.5 0.301*
Positron Beam Parameters at the target
By O. DADOUN
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Adiabatic Matching Device
• Length: L = 20-50 cm• Magnetic field at the
target : B0 = 6 T
• Magnetic field at the end : B(L) = 0.5 T
• Magnetic Field Behaviour :
zz
1
B)B(
0
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AMD RESULTS
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AMD
cm
N*. e+
Yield
e+/e-
x
mm mrad
y
mm mrad
<E> MeV
E
MeV
z *
mm
z
cm MeV
20 16476 2.75 682 681 78.9 164.7 8.7* 136.2
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CAVITY 100 KW CW (P. Lepercq)
L= 58.96886 cm Fr = 1.99915469674 GHz Iris : r = 20mm Ezmax(r=0)= 5.2 MV/m
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Capture Section Design
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e+ (200 MeV)
Target
AMD
e-
63 Cavities
Solenoid
AMD
• Length : L = 20 cm• Magnetic Filed: B = 6 - 0.5 T• Final Aperture: r = 2 cm
SOLENOID
• Length : L = 41 m• Magnetic Filed: B = 0.5 T• Drift Tube Aperture: r = 2 cm
Accelerating cavities:
• Number of cavities: N = 63• Length: L = 60 cm• Max Energy Gain: E = 5.95 MeV• Maximum Gradient: Ez (r=0) = 25 MV/m• Frequency: = 2 GHz
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Capture Results
20/04/23 A. Vivoli, CLIC Positron Source, CLIC 2009, CERN
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S
cm
N. e+
Yield
e+/e-
x
mm mrad
y
mm mrad
<E> MeV
E
MeV
z
mm
z
cm MeV
4200 6186 1.03 6939 7051 214.1 35.0 9.9 33.5
To be optimized…
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20/04/23 A. Vivoli, CLIC Positron Source, CLIC 2009, CERN
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Capture Section (+ Bunch Compressor)
Crystal To the accelerator
Target
Adiabatic MatchingDevice Pre-accelerator
Chicane
e-
e+
Solenoid Cavities
BendingMagnets
Drift
Magnetic field
Electric field
e+
e-
e-
Magnet LINAC 2 GHz
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e+
Magnetic Chicane
Quadrupoles
Bunch Compressor Design
TW structure
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Bunch Compressor Elements
Quadrupoles:
• Number: N = 14• Length: L = 20-40 cm• Gradient: G = 1.5 – 4.7 T/m• Aperture: r = 5-15 cm
Accelerating cavities:
• Number of cavities: N = 1 TW• Length: L = 3.9 m• Average Gradient: Ez = 14.5 MV/m• Frequency: = 2 GHz
Bending Magnets:
• Number: N = 4• Length: L = 30 cm• Magnetic Field: B = 0.3513 T
Drift Tubes:
• Number: N = 28• Aperture: r = 5-10 cm• Length: L = 10 - 40 cm
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MAGNETIC CHICANE
BS1 BS2 BS3 BS4
103
mm
for
=
172
mra
d
e+
0.30 m 0.30 m 0.30 m0.30 m
0.296 m 0.296 m0.30 m
- -
20/04/23 A. Vivoli, CLIC Positron Source, CLIC 2009, CERN
Chicane Modeling:
• Bending angle: = 9.87 deg• Drift: = 30 cm• Diaphragm: r = 4.0 cm
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Bunch Compressor Results
20/04/23 A. Vivoli, CLIC Positron Source, CLIC 2009, CERN
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S
cm
N. e+
Yield
e+/e-
x
mm mrad
y
mm mrad
<E> MeV
E
MeV
z
mm
z
cm MeV
5688 5895 0.98 22678 23479 211.8 26.0 7.7 18.35
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Injector Linac I (800 MeV)
TW structures
Quadrupoles
From A. Ferrari et al., CLIC Note 626-655-723
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Injector Linac II (1.5 GeV)
TW structures
Quadrupoles
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Injector Linac III (2.86 GeV)
TW structures
Quadrupoles
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Injector Linac Elements
Quadrupoles:
• Number: N = 196• Length: L = 40-60 cm• Gradient: G = 1.0 – 18.5 T/m• Aperture: r = 5-15 cm
Accelerating cavities:
• Number of cavities: N = 49 TW• Length: L = 3 - 4.5 m• Average Gradient: Ez = 14.5 MV/m• Frequency: = 2 GHz
Drift Tubes:
• Number: N = 50• Aperture: r = 5 cm• Length: L = 200 - 280 cm
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Injector Linac Results
S
cm
N. e+
Yield
e+/e-
x
mm mrad
y
mm mrad
<E> MeV
E
MeV
z
mm
z
cm MeV
38550 4558 0.76 19804 14729 2825.1 129.5 6.2 69.5
To be optimized…
e+ in PDR: 2747; Yield e+/e- =0.458
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Conclusions
• In order to have 4.6 109 e+ in PDR we need:
4.6 109/0.458=10 109 e- in primary electron beam on crystal.
• According to Dadoun et al., CLIC Note in preparation:
PEDD = 22.14*10 109 / 7.5 109 = 29.5 J/g < 35 J/g but close.
• Optimization of the parameters for non-polarized positrons is necessary and will be done soon.
• Configuration at 500 GeV and double charge not possible with only 1 fixed tungsten target for the moment.
• Utilization of different codes for simulations (PARMELA, PLACET, GEANT4,…) will be done.
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20/04/23 A. Vivoli, CLIC Positron Source, CLIC 2009, CERN
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THANKS.
The EndThe End