Studies of cERL injector Thursday, March 4, 2010 SLAC National Accelerator Laboratory Menlo Park, California Tsukasa Miyajima 7 th division, Accelerator Laboratory, KEK, High Energy Accelerator Research Organization ICFA Advanced Beam Dynamics Workshop on Future Light Sources Contents 1.Outline of compact ERL injector 2.Beam Simulation to optimize beamline parameters 3.Test beamline for cERL injector 4.Future issues 5.Summary
48th ICFA Advanced Beam Dynamics Workshop on Future Light Sources. Studies of cERL injector. Thursday, March 4, 2010 SLAC National Accelerator Laboratory Menlo Park, California Tsukasa Miyajima 7 th division, Accelerator Laboratory, KEK, High Energy Accelerator Research Organization. - PowerPoint PPT Presentation
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Studies of cERL injectorThursday, March 4, 2010
SLAC National Accelerator LaboratoryMenlo Park, California
KEK, High Energy Accelerator Research Organization
48th ICFA Advanced Beam Dynamics Workshop on Future Light Sources
Contents1.Outline of compact ERL injector2.Beam Simulation to optimize beamline parameters3.Test beamline for cERL injector4.Future issues5.Summary
ERL collaboration team• High Energy Accelerator Research Organization (KEK)
– M. Akemoto, T. Aoto, D. Arakawa, S. Asaoka, A. Enomoto, S. Fukuda, K. Furukawa, T. Furuya, K. Haga, K. Hara, K. Harada, T. Honda, Y. Honda, T. Honma, T. Honma, K. Hosoyama, M. Isawa, E. Kako, T. Kasuga, H. Katagiri, H. Kawata, Y. Kobayashi, Y. Kojima, T. Matsumoto, H. Matsushita, S. Michizono, T. Mitsuhashi, T. Miura, T. Miyajima, H. Miyauchi, S. Nagahashi, H. Nakai, H. Nakajima, E. Nakamura, K. Nakanishi, K. Nakao, T. Nogami, S. Noguchi, S. Nozawa, T. Obina, S. Ohsawa, T. Ozaki, C. Pak, H. Sakai, S. Sakanaka, H. Sasaki, Y. Sato, K. Satoh, M. Satoh, T. Shidara, M. Shimada, T. Shioya, T. Shishido, T. Suwada, T. Takahashi, R. Takai, T. Takenaka, Y. Tanimoto, M. Tobiyama, K. Tsuchiya, T. Uchiyama, A. Ueda, K. Umemori, K. Watanabe, M. Yamamoto, Y. Yamamoto, S. Yamamoto, Y. Yano, M. Yoshida
• Japan Atomic Energy Agency (JAEA)– R. Hajima, R. Nagai, N. Nishimori, M. Sawamura
• Institute for Solid State Physics (ISSP), University of Tokyo– N. Nakamura, I Itoh, H. Kudoh, T. Shibuya, K. Shinoe, H. Takaki
• UVSOR, Institute for Molecular Science– M. Katoh, M. Adachi
• Hiroshima University– M. Kuriki, H. Iijima, S. Matsuba
• Nagoya University– Y. Takeda, T. Nakanishi, M. Kuwahara, T. Ujihara, M. Okumi
• National Institute of Advanced Industrial Science and Technology (AIST)– D. Yoshitomi, K. Torizuka
• JASRI/SPring-8– H. Hanaki
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 2
The Compact ERL for demonstrating ERL technologies
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 3
Parameters
Beam energy 35 - 245 MeV
Injection energy 5 MeV
Average current 10 - 100 mA
Acc. gradient (main linac)
15 MV/m
Normalized emittance
0.1 - 1 mm·mrad
Bunch length(rms)
1 - 3 ps (usual)~ 100 fs (with B.C.)
RF frequency 1.3 GHz
Parameters of the Compact ERL
Before constructing large-scale ERL facility, we need to demonstrate the generation of ultra-low emittance beams using key devices.
Compact ERL
East Counter Hall
100 m
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 4
cERL injector• cERL injector: to generate electron beam with lower emittance and
shorter bunch length
Compact ERL
Parameters of the Compact ERL Injector
Photo cathode DC gun
Super conducting cavity(2 cell, 3 modules)
Merger section
ERL Injector
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 5
Components in ERL injector① Photo cathode DC gun
Gun, HV power supply, driving laser system② Solenoid magnet
To compensate emittance③ Bunching cavity
Normal conducting cavity for bunching④ SRF cavities
2-cell, 3 modules⑤ Quadrupole magnets
To adjust CS parameters before merger section⑥ Merger section
Physics in ERL injector(1) Space charge effect ( Coulomb force between electrons)(2) Solenoid focusing ( Emittance compensetion )(3) RF kick in RF cavity(4) Higher order dispersion in merger section(5) Coherent Synchrotron Radiation (CSR) in merger section(6) Response time of photo cathode ( It generates tail of emissio
n. )
These effects combine in the ERL injector.
The simulation code have to include(1)External electric and magnetic field, (2)Space charge effect (3D space charge).
To obtain high quality beam at the exit of merger, optimization of beamline parameters is required.
Method to research the beam dynamics: Macro particle tracking simulation with space charge effect is used.
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 8
Beam Simulation
Particle tracking code : GPT(General Particle Tracer)[1]Space charge calculation : 3D mesh based methodInitial particle distribution : beer-canNo CSR effect in merger section
• Purpose of simulation– To find optimum beamline parameters, i.e. magnet strength, RF phase, etc., with lower
emittance and shorter bunch length.– To calculate beam parameters, i.e. emittance, beam size, etc., to design components in ERL
injector.
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 9
Multi objective optimization• To minimize both emittance and bunch length at 1 m from the exit of merger• Multi objective method is used[2]
Free parameters in the optimization①Initial laser radius (mm)②Initial laser pulse length (ps)③Magnetic field of 1st solenoid④Electric field of bunching cavity⑤Magnetic field of 2nd solenoid⑥Electric field and phase of SRF1⑦Electric field and phase of SRF2⑧Electric field and phase of SRF3⑨Magnetic fields of 5 quadrupoles
[2] Ivan V. Bazarov and Charles K. Sinclair , Phys. Rev. ST Accel. Beams 8, 034202 (2005).
Number of free parameters: 16 Minimize both emittance and bunch length. (2 objects optimization)
Layout of beamline
Beam parameters are calculated at 1 m from exit of merger.
Results of optimizationBunch length vs. normalized rms emittanceFor shorter bunch length, emittance is larger than the case of longer bunch length.
Normalized rms emittance0.4 ~ 0.5 mm mrad
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 10
Dependence on number of particles• In the macro particle tracking simulation, we can not avoid the effect of number of macro particles,
because we can not simulate actual number of electrons.
• To obtain more accurate results, – In early optimization : 5k particles ( to save CPU time )– But, the accuracy is not so good for 5 k particles– In final optimization, we optimize beam line parameters with 200 k particles after the early optimization with
5k particles.
Normalized rms emittance Rms beam size
At lease Nps > 100 k
For 77 pC, actual number of electrons is 480 M particles.
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 11
Optimum beamline parameters• Beam line parameters for high current mode with 80 pC/bunch, which give bunch
length of 0.63 mm and normalized rms emittance of 0.56 mm mrad
*:RF phase from maximum acceleration.
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 12
Time evolution of beam parameters(1) Normalized rms emittance (2) Rms beam size and bunch length
(3) Kinetic energy and energy spread
Normalized rms emittance : 0.56 mm mradBunch length : 0.63 mmKinetic energy : 8.2 MeVRelated rms energy spread: 0.23 %
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 13
Time evolution of phase space distributioncathode
1st solenoid
2nd solenoidBunching cavity Exit of SRF 5 quadrupoles
Exit of merger
Bunch charge: -80 pC/bunchNormalized rms emittance : 0.56 mm mradBunch length : 0.63 mmKinetic energy : 8.2 MeV
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 14
Summary of optimization• We have designed the injector for the cERL and carried out beam
dynamics simulation using the particle tracking code with 3D space charge effect.
• To optimize the beamline parameters, we are using multi objective method and cluster linux machine.
• At the end of the injector, we have obtained the emittance of 0.56 mm·mrad with the bunch length of 0.63 mm for the high current operation mode (80 pC/bunch).
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 15
Gun test beamline for cERL injector
NPES3, 200 kV guntransferred from Nagoya university at May 2009.
Gun Test beamline
Test area for 500 kV gun
Laser system
• Purpose of test beam line– To gain operation experience of the low energy beam.– To evaluate performance of the DC guns by an additional diagnostic line to measure
emittance and bunch length– To develop a new 500 kV gun, diagnostic system and the injector line used at cERL.
2010- middle of 2011: 200 kV gun2011 - : new 500 kV gun
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 16
Layout of gun test beamline
1st solenoid2nd solenoid
3rd solenoid 4th solenoid
1st view screen2nd view screen
1st slit(vertical)
1st slit(horizontal)
2nd slit(vertical)
2nd slit(horizontal)
The same layout as cERL injector Beam diagnostic line (emittance, Bunch length measurements)
Beam dump line
3rd view screen 4th view screen
5th view screen
deflectorBending magnet
Beam dump
Components for gun test facility• We are constructing gun test facility with 200 kV photo cathode DC gun in AR south experimental
hall, KEK. From this spring, we are going to start beam running.
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 17
Two solenoid magnets
Laser chamber
1st solenoid
2nd solenoid
Laser chamber
1st view screen monitor
2nd view screen monitorBunching cavity
From Gun
To SRF cavity
e-
e-
The layout of the cERL injector before SRF cavity.In the first test, the bunching cavity is not installed.
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 18
Beam dynamics of gun test beamline Initial parameters at point A:① Radius of initial particle
distribution : 1.91 mm② Laser pulse full width : 41.5 ps③ 1st Solenoid : 0.039 T④ Bunching cavity : 0 kV⑤ 2nd Solenoid : 0.026 T
Gun 1st view screen 2nd view screen
1st slit 3rd view screen
A
Result of optimization
At 1st slit, Emittance: 0.42 mm mradBunch length: 6.7 mm
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 19
Future issues• Beamline parameter optimization for XFEL-O with 20 pC, 0.1 mm mrad.
– To obtain lower emittance, can we increase the voltage of the photo cathode gun over 500 kV?
• Beam optics matching with return loop• Establish the beam tuning method in the commissioning. • Beam simulation with CSR and Space charge effect in the merger section.
We developed CSR routine, which is effective in lower energy beam.
cf. K.-J. Kim et al., PRL 100, 244802 (2008).
R. Hajima and N. Nishimori (JAEA), Proc. FEL2008, pp. 87-89.
Beam simulation for XFEL-O• Target values for XFEL-O: < 0.1 mm mrad, 20 pC/bunch, 2 ps bunch length
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 20
Layout of beamline
Beam parameters are calculated at 1 m from exit of merger.
(1) 0.6 mm (2 ps) bunch length enx = 0.14 mm mrad with 500 kV enx = 0.13 mm mrad with 600 kV
(2) 0.9 mm (3 ps) bunch length enx = 0.12 mm mrad with 500 kV enx = 0.11 mm mrad with 600 kV
It is not so far from target value for XFEL-O. We are going to investigate the effect of gun voltage.
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 21
Summary• Beam dynamics simulation for the cERL has been carried out using 3D space
charge macro-particle tracking code. • To find the optimum parameters, which give minimum emittance and bunch
length, the parameter optimization has been carried. • For high current mode with 80 pC/bunch, we obtained the minimum emittance of
0.56 mm mrad with the bunch length of 0.63 mm.
• To design ERL components (Gun, Buncher, SRF cavities, solenoid, alignment, etc.), we have studied tolerances of errors in ERL injector.
• To evaluate performance of the DC guns, we are developing the gun test beamline in the PF-AR south experimental hall.
• From the early part of March, we are going to start beam running in the gun test beamline using NPES3 200kV DC photo cathode gun.
• For XFEL-O, the minimun emittance is calculating with 20 pC/bunch.• So far, we have obtained the minimum emittance of 0.13 mm mrad with the
bunch length of 0.6 mm (2 ps) and the gun voltage of 600 kV.
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 22
Backup slides
Effect of gun voltage
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 23
(1) 0.6 mm (2 ps) bunch length enx = 0.14 mm mrad with 500 kV enx = 0.13 mm mrad with 600 kV
(2) 0.9 mm (3 ps) bunch length enx = 0.12 mm mrad with 500 kV enx = 0.11 mm mrad with 600 kV
Preliminary resultsBunch charge: 20 pC/bunchGun voltage: 500 kV or 600 kVAt exit of merger
Results of Gun and solenoid beamline
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 24
How to optimize the parameters?• Macro particle tracking simulation with space charge requires longer CPU time. • In the optimization, tracking simulation is repeated to search optimum parameter.
Therefore, the calculation time to optimize the parameters is too long.
• To save the calculation time, efficient optimization method is required. • In order to reduce the calculation time, we use
– Multi objective method [2] as an efficient method, and– Cluster linux computer, which have 80 CPUs. The parallel 80 jobs, which have different
beamline parameters, can be executed on the cluster computer.
To minimize emittance and bunch length
Trade-off solutions
Two objects in the optimization1.Emittance2.Bunch length
[2] Ivan V. Bazarov and Charles K. Sinclair , Phys. Rev. ST Accel. Beams 8, 034202 (2005).
Tsukasa MiyajimaFLS2010, March 1-5, 2010,
SLAC National Accelerator Laboratory 25
Results of optimization(1) Sector type ( bending angles : -19, 22, -19 degree)
Emittance growth caused by space charge dispersion. The rectangular type gives smaller emittance than the sector type. It seems that stronger longitudinal space charge dispersion in the sector type causes the difference of emittance, because the bending angle of the bending magnet in the sector type (19◦ or 22◦) are larger than one in the rectangular type (16◦).
(a) Maximum emittance growth(b) Minimum emittance growthEmittance growth depends on space charge dispersion.
Beam parameter with 7.7 pC/bunch• Charge: 7.7 pC/bunch• Emittance: 0.097 mm mrad (horizontal), 0.090 mm mrad(vertical)• Bunch length: 1.3 ps
• Merger section• Original routine (spacecharge3dmesh) ⇒ calculated emittance is not correct.• It is clear for smaller number of particles.
• We checked the source code.
orbit( in drift space )
emittanceCalculated emittance depends on angle from z-axis.
Why?
Injected beam
Beam goes forward along the following orbit.
Enhanced space charge calculation in GPT• In original spacecharge3dmesh routine, direction of mesh box : fixed to coordinate in GPT• When beam go forward along oblique line fro z-axis, mesh size becomes coarse.
We made enhanced routine ⇒ spacecharge3dmeshxz
Original
Enhanced routine
Spacecharge3dmeshxzThe enhanced routine can calculate the accurate emittance.
Misalignment of solenoid• Misalignment of solenoid position and angle
35
The beam parameters are calculated at exit of SRF cavities.
Result 1: Ripple of Gun HV source• Arrival time• 0.1% error: -120 fs
10 June, 2009 ERL09 36
• Normalized rms emittance• ±0.1% error: fluctuation of 3.5 %
• Kinetic energy• 0.1% error:
99.96%
Timing in buncher
10 June, 2009 ERL09 37
Result 2: Amplitude error in RF cavities
10 June, 2009 ERL09 38
• Normalized rms emittance• ±0.1% error: fluctuation of 1.5 %