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Undulator Based Positron Sources. Mike Jenkins Lancaster University and The Cockcroft Institute. Presentation Overview. Positron source requirements of future colliders Undulator based positron source design Current undulator developments Update on Target material measurements. - PowerPoint PPT Presentation
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Mike JenkinsLancaster University and The Cockcroft
Institute
Presentation OverviewPositron source requirements of future
collidersUndulator based positron source designCurrent undulator developmentsUpdate on Target material measurements
06/04/2011 IOP NPPD Glasgow 2
Requirements of a Positron SourceThere are currently three proposed designs for particle accelerators which require a positron production rate of >1014 e+/s
Conventional solutions to produce positrons have a production limit of 6 x 1012 e+ /s
Collider Positron Production Rate (number of e+ /s)
ILC 3.9 x 1014
CLiC 1.1 x 1014
LHeC 3.1 x 1015
Future Positron Source DesignsCurrent proposed designs for the positron source at future colliders include:
laser-Compton based source
Undulator based
Hybrid Target (crystalline target and amorphous target)
06/04/2011 IOP NPPD Glasgow 4
Undulator Based Positron Source
Schematic of ILC RDR Positron Source
06/04/2011 IOP NPPD Glasgow 5
Length of Undulator
Number of γ / e-
Heat Load on Target
Number of e+ /e-
~150m to 250m 200 ~20 kW (beam)Up to 20 kW (eddy currents)
2
Undulator DevelopmentsCurrently the
superconducting undulator planned for use in the positron source is made using NbTi conductors
NbTi undulator prototype for ILC is currently being tested at RAL
Simulations into different superconductors are on going, the work presented here is based on Nb3Sn conductors
Parameter
Design Value
Test Results
Period 11.5 mm 11.6 mm
Field on Axis
0.86 T 0.88 T
Undulator Developments OP
ER
A 3
D S
imu
latio
n o
f Un
du
lato
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Flux Density: 0.070 T to 4.85 T
Undulator Developments
06/04/2011 IOP NPPD Glasgow 8
Positron Source Target
Courtesy of Ken Davies, Daresbury Lab
Courtesy of Jim Rochford, RAL
0.5 to 1.5 T Dipole Magnet
1 m Titanium Target
Eddy Current ResultsPeak Torque(Carmen)
Average Torque(Carmen)
Min Torque(Carmen)
Preliminary Data
Results for peak field of 0.5 T and target immersion depth of 30.25 mm
06/04/2011 IOP NPPD Glasgow 10
Target Material ConductivityTo resolve the difference between simulations and the data the properties of the titanium are being investigated.
Currently the electrical and thermal conductivity of the titanium is being measured
Expected Resistance
8.8 x 10-5 Ω
Expected Electrical Conductivity
5.62 x 105 S m-1
Expected Thermal Conductivity
6.70 W K-1 m-1
Target Material Conductivity
Samples
Probe 2
Probe 1
Sample Length (mm)
Width (mm)
Height (mm)
A 49.96 16.46 4.94
B 49.97 16.45 9.96
C 49.82 16.37 14.9206/04/2011 IOP NPPD Glasgow 12
Target Material Conductivity
Oxygen Free Copper Contacts
Springs
Sample06/04/2011 IOP NPPD Glasgow 13
Target Material ConductivityExperimental setup
consists of a AC current source and nanovoltmeter connected to LabView
Only preliminary DC measurements taken so far
Trying to understand systematic effects causing shifts in the signal between consecutive data taking periods
SummaryUndulator simulations are promising, it
appears that the new wire could allow the undulator period to reduce from 11.5 mm to 10.0 mm keeping K constant
Awaiting confirmation about the performance of the Nb3Sn wire, current uncertainty about the performance of the wire at low field strength
Conductivity measurements of the target material are preliminary and there are a few issues still to resolve
06/04/2011 IOP NPPD Glasgow 15
Thank you for listening, are there any questions