electron and positron source - linear collider
TRANSCRIPT
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Electron and Positron source
KEK M. Fukuda
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 1
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International Linear Collier (ILC)
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 2
Positron source:Undulator scheme: E-driven scheme
125GeV e+ Beam
125GeV e- Beam Electron source: Polarized electron
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2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 3
Electron source
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Beam parameters for the electron source
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 4
ILC-TDR
ILC requires the following electron beams:
Bunch charge: 2.0x1010 e-/bunch (3.2nC/bunch)Number of bunches: 1312bunches/trainRep. Rate: 5HzPolarization: >80%
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Layout of the polarized electron source
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 5ILC-TDR
- Electrons are generated by using a 200 kV DC gun with a NEA-GaAs cathode.- The 325MHz subharmonic buncher (SHB) compresses the bunch length.(1ns20ps)- Electrons are accelerated to 76 MeV with an L-band TW accelerator in a solenoid
magnetic field.- After passing chicane for energy collimation, electrons are accelerated to 5GeV
with superconducting linac.- A spin rotator rotates the spin in the vertical direction and electrons are injected to
the damping ring.
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Polarized electron generation
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ILC-TDR
Strained GaAs/GaAsP superlattice photocathodeQuantum efficiency (QE): 0.3~0.5% (max. 1%)Polarization: > 85%
Polarizedelectron
Circular polarized laser light
QE: 0.5% , Polarization: 92% : T. Nakanishi: Proceeding of LINAC2002, 813 (2002).
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Polarized electron generation
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 7
-1/2 1/2
-1/2 1/2
-1/2 1/2 3/2-3/2
-1/2 1/2
-1/2 1/2
-1/2 1/23/2-3/2
(3) (1)
Valence band
Conduction Band
Unstrained GaAs Strained GaAs
Polarization > 90%Polarization 50%(Max)
Eg: 1.43eV
ΔE 0.34eV ΔE 0.05eV
Polarization = (N+ - N-) / (N+ + N-)
Unstrained GaAs Strained GaAs: Polarization is increased.
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NEA(Negative Electron Affinity)
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 8
Xiuguang JIN,「加速器」Vol. 16, No. 1, 2019(22–27)
NEA surface is made by deposition of Cs and O on GaAs surface. Quantum efficiency (QE) is increased.
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GaAs/GaAsP strain-compensated superlattice
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 9Xiuguang JIN,「加速器」Vol. 16, No. 1, 2019(22–27)
Strained Superlattice: Polarization 92%, QE: 0.5%Thickness ~100nm Absorption of the laser light: 4-5%
Strain-compensated superlattice: Thickness : 720nm Polarization 92%, QE: 1.6%
Xiuguang Jin, et.al., “Effect of crystal quality on performance of spin-polarized photocathode”, Appl. Phys. Lett, Applied Physics Letters, 105(20):203509, 2014.
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200kV DC high voltage photogun
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 10
DC High voltage: 200kVPhotocathode: Strained-superlattice GaAs/GaAsP
To reduce the space charge effect which make the emittance worse, the high voltage is needed.
ILC-TDR
Average current : 4mA
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cERL DC gun
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 11
Generation of a high-current beam greater than 0.8 mA at 500 kV for approximately 2 h was demonstrated.
N. Nishimori et.al., “Operational experience of a 500 kV photoemission gun”, PHYS. REV. ACCEL. BEAMS 22, 053402 (2019)
A 500kV DC electron gun is operated in compact-ERL at KEK.
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Gun laser system
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 12
To match the bandgap energy of GaAs photocathodes, the wavelength of the laser system must be 790 nm and provide tunability (±20 nm) to optimize conditions for a specific photocathode. Therefore, the laser system is based on Ti:sapphire technology.
ILC-TDR
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Bunching and Pre-Acceleration
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 13
The bunching system compresses the 1 ns micro-bunches generated by the gun down to 20 psTo avoid the surface-charge-limit problem, the bunch length is 1ns at the DC gun.
SHB(Subharmonic buncher) (325MHz) x2, 1ns 200psL-band Buncher (5cells), 200ps 20ps
The e- beam is accelerated to 76MeV by the L-band normal conducting TW accelerator.
OHO13 T. Asaka
OHO02, H.Sakai
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5GeV linac to Damping Ring
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 14
After the Pre-Acceleration、an e- beam is accelerated to 5GeV by the Superconducting linac which consists of 24 cryomodules. That cryomodules are drived by eight 10MV klystrons .The Linac To Ring (LTR) beam line transports the beam to the injection point of the damping ring.
Bend7.93deg
The electron spin component in the plane normal to the applied magnetic field will precess 90deg in that plane for every 7.93deg of rotation of the momentum vector at 5GeV.
K. Moffeit, et.al. , SLAC-TN-05-045
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Simulation
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 15
Simulations indicate that >95% of the electrons produced by the DC gun are captured within the 6-D damping ring acceptance: γ(Ax+Ay) <=0.07 m and ΔE×Δz <=(±37.5 MeV)×(±3.5 cm). The starting beam diameter at the gun is 2 cm, which is focused to a few mm diameter before it is injected into the DR.Simulation code: PARMELA、MAD、 ELEGANT code [81].
ILC-TDR
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2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 16
Positron source
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Positron production
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 17
・β+ decayP+ n + e+ + νe
・Pair productionPhotons interact with the nuclear Coulomb field and produce electron-positron pairs.Photons with energy of more than 1.022MeV are required.
阪井寛志、OHO02
Pair generation is used as a positron beam source.Since it accelerates by the electric field, bunched positrons are required. Bunched gamma-rays can make the bunched positrons by pair production.
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Cross section of pair production
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 18
The Review of Particle Physics (2018)M. Tanabashi et al. (Particle Data Group), Phys. Rev. D 98, 030001 (2018),http://pdg.lbl.gov/
Gamma rays of about 10 MeV or more are useful for generating positron beams.
- The cross-section rises from 1.022MeV, and the increase becomes moderate at 10-100MeV or more.
- The cross-section of pair production is proportional to the square of atomic number Z.
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Positron beam production method
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 19
OHO’07, T. Kamitani
Target material・E-driven scheme- The electromagnetic shower is used when the
electron beam is injected to the material.- The bremsstrahlung and pair production are
repeated to generate many electrons, positrons, and photons.
- Unpolarized positrons
・Undulator scheme- Positrons are generated by pair production
when gamma rays generated by a helical undulator are injected to a target material.
- Electromagnetic shower hardly occurs (a thin metal target is used.)
- Circularly polarized gamma rays can generate a polarized positron beam.
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ILC positron beam
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 20
Undulator scheme E-driven scheme
Report on the ILC Positron Source, Positron working group
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Undulator scheme
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 21
ILC - Technical Design Report(TDR)
- Gamma-rays from helical undulator drived by 125GeV e- beam is injected and positrons are generated by pair production.
- Rotating target, Material: Ti alloy- Matching device : QWT - Positrons are accelerated up to 400MeV in the capture linac and the pre-accelerator.- Positrons are accelerated up to 5GeV by SC booster.- A spin rotator rotates the spin in the vertical direction and electrons are injected to the
damping ring.- ECS reduced the energy spread for matching to DR aperture.
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Gamma-ray generation using helical undulator
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 22
The electron beam energy was changed to 125 GeV.Gamma-rays energy is also reduced from 10 MeV to 7 MeV. It causes the reduction of the intensity of gamma-rays because the cross section of pair production is decreased.Therefore, the length of undulator is extend from 147 m to 231m.
Undulator prototypemade in CockcroftK=0.92 , λu 1.15cm、Inner diameter: 5.85mm
Phys. Rev. Lett 107 (2011) 174803Energy [MeV]
Energy distribution of gamma-rays
7MeV
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Positron polarization
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 23
The polarization of gamma rays correlates with energy and scattering angle.Higher polarization is derived by choosing higher energy gamma-rays.Polarization : 30 – 60%
K. Yokoya, ILC Camp 2012
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Rotating target (Undulator scheme)
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 24
A rotating target is used to reduce the thermal load on the target.
LCWS2017, S. Riemann
Average temperature< 460℃
Rotating target:Material: Ti alloy(Ti6Al4V), thickness 7mmWeight: ~50kgDiameter: 1mRotation speed: 100m/s (~2000 rpm)Bearing: magnetic bearingCooling:Radiation coolingHeat load: 2kW
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Rotating target
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 25
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Optimization of Target thickness
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 26
e- 125GeV, 1312bunchesK = 0.85
The electron beam energy was changed to 125 GeV.- Gamma-rays energy is also reduced from 10 MeV to 7 MeV.- Undulator length: 147 m 231m to increase the intensity of gamma-rays.- Heat load is increased.
The thickness of the Ti alloy is reduced from 14 mm to 7 mm because the positron yield is almost unchanged.The heat load is also reduced to 1/3.
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Optical matching device
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 27
The positron is captured by a strong solenoid magnetic field excited by a pulse current.
Optical matching device: Small beam size, Large divergence
↓Large beam size, Small divergence
There are two method, QWT or AMD.
QWT
QWT(Quarter wave transformer) AMD(Adiabatic matching device)
or ガンマ線
OHO’07, T. Kamitani
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・QWT - The QWT transforms 90deg in the phase space.
It captures the positrons satisfying this condition.
- Energy acceptance is narrow.
Kamitani20061101.pdfPrimary coil
Conductor
e+e-
Optical matching device(OMD)
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OHO07, Kamitani
Flux concentrator
CERN-94-01
Adiabatic invariant
Magnetic field: BiQWT length: Li Momentum: pz
・AMD- AMD field is produced by a flux-concentrator.- The eddy current is induced in the tapered
conductor which makes the strong magnetic field.- Energy acceptance is large.
adiabatic condition
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OMD for undulator scheme
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In ILC TDR, the matching device is flux concentrator.・The strength of the magnetic field could not be maintained for 0.7 ms.・Energy deposition is too large due to a small aperture (13mmφ). Now we are considering using QWT.
Designed by Wanming Liu
FocusingBacking
To prevent eddy currents on the rotating target, a reverse polarity backing coil is placed.Magnetic field on the target is zero.
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Capture section
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LCWS2017, A. Ushakov
After the QWT, there is the capture section which consist of 2 SW accelerators and 11 TW accelerators.These accelerators are put in the solenoid field.
Deceleration phase captureWhen positrons are put on the deceleration phase, the number of captured positrons increases.
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Positron Yield for Undulator scheme
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 31Analyzed by T. Okugi
Number of positron in DR Number of primary electronsYield (e+/e-) =
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Positron Yield for Undulator scheme
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 32
Input magnetic field
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E-driven scheme
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- 3GeV e- beam is injected to the target and positrons are generated by an electromagnetic shower.
- Rotating target, Material: W26Re- Matching device : Flux concentrator - Positrons are accelerated up to 250MeV in the capture linac.- Chicane compresses the bunch length.- Positrons are accelerated up to 5GeV by L-band and S-band NC accelerators.- ECS reduced the energy spread for matching to DR aperture.
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Pulse structure
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 34
33bunches x 40 = 1320
ALCW2018, M. Kuriki
100Hz33bunches x 2
Heat load is too large.
1312bunches (~1ms)
..…
Target
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Beam extraction from DR
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Target
36
RequirementsHigh Z (Cross section of Bremsstrahlung ∝ Z2/A)High melting pointTantalum(73Ta), Tungsten(74W), Tungsten- rhenium alloy (W-Re)
ILC: Target material: W26Re 16mm (~4χ0)
Summer camp on ILC accelerator, physics and detectors 2019OHO’07, T. Kamitani2019/09/05
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Rotating target
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 37
W-Re 16mm3.0GeVσx,y: 2mm33+33bunches
ALCW2018, T. Omori
Rotating target:Material: W26Re, thickness 16mmWeight: ~70kgDiameter: 0.5mRotation speed: 5m/s (~225 rpm)Vacuum seal: ferrofluid sealCooling:Water cooling, 60L/minHeat load: 16kW
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Ferrofluid seal
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 38
http://www.rigaku-mechatronics.com/technology/
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Heat load for Rotating target
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 39
Report on the ILC Positron Source, Positron working group
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Optical matching device (E-driven)
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 40ILC夏の合宿2017, M. Kuriki
Flux concentrator is used in E-driven scheme.
Report on the ILC Positron Source, Positron working group
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Capture section
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 41
J. W. Wang SLAC-PUB-12412
Positrons are accelerated to 250 MeV by 36 L-band SW accelerator tubes surrounded by 0.5 T solenoid field.
The aperture of the acceleration tube is 60mm in diameter.
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Number of positrons at the end of capture section (250MeV)
2019/09/05
Summer camp on ILC accelerator, physics and detectors 2019 42
The phase of accelerating field is scanned to find the maximum point of number of positrons.
Num
ber o
f pos
itron
s at
the
exit
of th
e ca
ptur
e se
ctio
n
Decelerating Phase352deg
Accelerating phase172deg
Focused by Bφ Defocused by Bφ
The best phase is +30deg from the decelerating phase. 20deg in this graph.
Positrons within +/-7mm from the peak of longitudinal position distribution are captured in DR.
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Booster section
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Positrons are accelerated to 5 GeV by L-band and S-band TW accelerator tubes.
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Beam loading compensation
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 44
Accelerating voltage(No beam )
Beam loading
Accelerating voltage+ Beamloading
ILC夏の合宿2017, M. Kuriki
Positrons are accelerated by doublet multi-bunch pulse.
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Energy Compressor Section(ECS)
2019/09/05 Summer camp on ILC accelerator, physics and detectors 2019 45
Positron Yield in DR: Y(e+/e-) : 1.3Z: longitudinal position、δ: エネルギー偏差
第15回高輝度・高周波電子銃研究会、名越久泰
ECS reduces the energy spread. Damping ring acceptance: ΔE×Δz <=(±37.5 MeV)×(±3.5 cm).
Chicane x 3 3m L-band SW x 4
Low energy positrons will delay after passing chicanes.The energy in a bunch is modulated by RF in accelerating tubes.
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Summary• Electron source
• The design by simulation of the electron source is basically completed.
• Strain-compensated superlattice GaAs/GaAsP, Pol. 92%, Q.E. 1.6%
• 500kV DC electron gun• Positron source
• Undulator scheme, E-driven scheme• Both schemes continue to optimize the design through
simulation.• Tunnel design including arrangement of beamline, radiation
shield and so on is under consideration.
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