Download - ERL Compton scheme for CLIC
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ERL Compton scheme for CLIC
L. Rinolfi (CERN) and T. Omori (KEK)many thanks to all Posipol collaboraters
CLIC WS 15-Oct-2009 CERN
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Collaborating Institutes:BINP, CERN, DESY, Hiroshima, IHEP, IPN, KEK, Kyoto, LAL, CELIA/Bordeaux, NIRS, NSC-KIPT,
SHI, Waseda, BNL, JAEA and ANL Sakae Araki, Yasuo Higashi, Yousuke Honda, Masao Kuriki, Toshiyuki Okugi, Tsunehiko Omori, Takashi Taniguchi, Nobuhiro Terunuma, Junji Urakawa, Yoshimasa Kurihara, Kazuyuki Sakaue,
Masafumu Fukuda, Takuya Kamitani, X. Artru, M. Chevallier, V. Strakhovenko, Eugene Bulyak, Peter Gladkikh, Klaus Meonig, Robert Chehab, Alessandro Variola, Fabian Zomer,
Alessandro Vivoli, Richard Cizeron, Viktor Soskov, Didier Jehanno, M. Jacquet, R. Chiche, Yasmina Federa, Eric Cormier, Louis Rinolfi, Frank Zimmermann, Kazuyuki
Sakaue, Tachishige Hirose, Masakazu Washio, Noboru Sasao, Hirokazu Yokoyama, Masafumi Fukuda, Koichiro
Hirano, Mikio Takano, Tohru Takahashi, Hirotaka Shimizu, Shuhei Miyoshi, Yasuaki Ushio, Tomoya Akagi,
Akira Tsunemi, Ryoichi Hajima, Li XaioPing, Pei Guoxi, Jie Gao, V. Yakinenko, Igo Pogorelsky, Wai Gai, and
Wanming Liu
World-wide PosiPol Collaboration
POSIPOL 2006CERN Geneve26-27 Aprilhttp://posipol2006.web.cern.ch/Posipol2006/
POSIPOL 2007LAL Orsay23-25 May
http://events.lal.in2p3.fr/conferences/Posipol07/
POSIPOL 2008Hiroshima16-18 June
http://home.hiroshima-u.ac.jp/posipol/
POSIPOL 2009Lyon23-26 Junehttp://indico.cern.ch/internalPage.py?pageId=1&confId=53079
POSIPOL 2010Tsukuba
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Two ways to get pol. e+(1) Helical Undurator
(2) Laser Compton
e- beam E >150 GeV
Undulator L > 200 m
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Two ways to get pol. e+(1) Helical Undurator
(2) Laser Compton
e- beam E >150 GeV
Undulator L > 200 m
Our Proposal
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Why Laser-Compton ?ii) Independence Undulator-base e+ : use e- main linac Problem on design, construction, commissioning, maintenance, Laser-base e+ : independent Easier construction, operation, commissioning, maintenance
v) Low energy operation (exsmpl: Ecm = 230 GeV) Undulator-base e+ : not suitable Laser-base e+ : no problem
i) Positron Polarization.
iii) Polarization flip @ 50 Hziv) High polarization
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Three of Compton schemes
for CLIC and ILC1. Ring-based Compton.
3. Linac-based Compton.
2. ERL-based Compton.
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Three of Compton schemes
for CLIC and ILC1. Ring-based Compton.
3. Linac-based Compton.
2. ERL-based Compton.
My talktoday
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ERL
laser pulse stacking cavities
positron stacking in main
DRRe-use Concept
to main linac
ERL Compton
efficient photon beam
efficient electron beam
e-Linac or E-gun
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31 MHz
325 MHz
Optical Cavity for Pulse Laser Beam
Stacking
Cavity Enhancement Factor = 1000 - 105
Laser-electronsmall crossing angle
Laser bunches
Lcav = n Lcav = m Llaser
Reuse high powerlaser pulse
by optical cavity
collision is not head-on
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injection 10 MeV RF-Gun
1.8 GeV 10 MeVdump 10 MeV
laser-pulse stacking cavity1.8 GeV 1.8 GeV -
E_loss
accelerating electron bunches(take energy from acc. cavities)decelerating electron bunches(give energy to acc. cavities)
gamma rays
ERL based Compton source
1.8 GeV - E_loss
10 MeV1.8 GeV
superconducting electron linac
E_loss : beam energy loss cased by Compton scatterings
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Points of ERL: 1Re use: Energy of electron beamThrow away: electron beam.
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Points of ERL: 1Re use: Energy of electron beamThrow away: electron beam.Points of
ERL: 2Fresh, high quality beam Small spot size (10 micron) at CP.
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Points of ERL: 1 Re use: Energy of electron beamThrow away: electron beam.Points of ERL:
2 Fresh, high quality beam
Beam compression (3 ps to < 1 ps)
Points of ERL: 3
Small spot size (10 micron) at CP.Short bunch (< 1 ps) at CP. (non head-on)
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injection 10 MeV RF-Gun
1.8 GeV 10 MeVdump 10 MeV
laser-pulse stacking cavity1.8 GeV 1.8 GeV -
E_loss
accelerating electron bunches(take energy from acc. cavities)decelerating electron bunches(give energy to acc. cavities)
gamma rays
ERL based Compton source
1.8 GeV - E_loss
10 MeV1.8 GeV
superconducting electron linac
E_loss : beam energy loss cased by Compton scatterings
decompressioncompression
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Points of ERL: 1 Re use: Energy of electron beamThrow away: electron beam.Points of ERL:
2 Fresh, high quality beam
Beam compression (3 ps to < 1 ps) Points of ERL:
4 Need steady exchange of energy: Accel-Bunches, Decel-Bunches, Klystrons Need CW operation
Points of ERL: 3
Small spot size (10 micron) at CP.Short bunch (< 1 ps) at CP.
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CLIC e+ source parameters
• 4.2 x 109 e+/bunch (exit of Pre Damping
Ring:PDR)
• E (PDR and DR) = 2.86 GeV• Tb-to-b = 0.5 ns
• CDR = CPDR ~ 400 m
• Nbunch = 312 / trian
• Frep = 50 Hz (Ntrain = 50/sec)
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ERL : CW device
CLIC : short pulse 150 ns & high
rep. 50 Hz
(312 bunches w/ 0.5 ns
spacing)
Compare ERL and CLIC
How to adapt ERL to CLIC?
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SolutionPut 2 stacking rings (SRs) between ERL and PDRto separate stacking and damping functions.ERL
C = 48mSR1
123
321
PDR
123312
47 m
C = 400
m
C = 48mSR2
123
321
Kill 321 - 312 = 9 bunches
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Configuration
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• C = 48.15 m• 0.156 s / turn• 321 bunches in a ring 321 x 0.5 ns x 0.3 m/ns = 48.15 m• stack in the same bucket every 64th turn
(injected beam: Tb-to-b = 32 ns -->
explain later )• N of stacking in the same bucket = 2003 64 x 2003 = 128 192 turns = 1.2 x 105 turns
0.156 s x 1.2 x 105 = 19.9979 ms 20 ms• "Stacking = 20 ms" + "Damping in SR = 20 ms" --> total 40 ms /cycle (25 Hz)
Stacking Ring (SR)
match
SR makes stacking and pre2 damping
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Stacking in a SR : part 1We give labels "1" to "321" to the buckets
in the SR. 123
64
SR
321
193
320
C = 48 m
25765
129
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• 1st turn 1 65 129 193 257
• 2nd turn 321 64 128 192 256
• 3rd turn 320 63 127 191 255••• 64th turn 2 66 130 194 258
• 65th turn 1 65 129 193 257
• 66th turn 321 64 128 192 256
•
Stacking in a SR : part 2
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ERL(CW)
Timing Chart
SR1(25Hz)
SR2(25Hz)
PDR(50Hz)
DR(50Hz)
stackdamp stackdamp stackdamp stack
stack
damp stack
damp stack
damp
0 20 40 60 80 100 120 140Time [ ms ]
to SR1 to
SR2
to SR1 to
SR2
to SR1 to
SR2
to SR1
to PDR to PDR to PDR
to PDR to PDR to PDR
from SR1from SR2
from SR1from SR2
from SR1from SR2
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• e- beam (ERL)
3 x 109 e-/bunch E = 1.8 GeV
• Laser 600 mJ / cavity 1 cavity in ERL
• 5 x 108 -rays/bunch
• 2.5 x 106 e+/bunch
• 5 x 109 e+/bunch (CLIC requires 4.2 x 109 )
Number of -rays/ e+s
collisio
n
thin conversion target: yield 0.5 %
2003 stacking in the same bucket
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• 3 x 109 e-/bunch
• E = 1.8 GeV• Tb-to-b = 32 ns
• Fref = 31.25 MHz
• FRF = 1 GHz (for example)
ERL
Accelerating bunchesDecelerating bunches
1 nsec (1 GHz)
Tb-to-b = 32 nsec
Tb-to-b = 32 nsec
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Summary
• Stacking ring with 48 m circumference and 1 GeV is also a challenge.
• A solution where stacking and damping are decoupled seems possible to fulfill CLIC requirements with an ERL scheme • Challenge remains to be demonstrated in order to make 2000 stacking in a same bucket. There was a simulation for ILC-ERL-Compton by F. Zimmerman. The result was encouraging.
• The cost increase with 2 storage rings is not an issue compared to the rest of the complex.
• ERL scheme can provide small spot size and short pulse at the laser-electron collision point. Especially short pulse (< 1ps) is big advantage.
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Backup slides
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Status of Compton Source
We still need many R/Ds and simulations.
We have 3 schemes. Choice 1 : How to provide e- beam Storage Ring, ERL, Linac Choice 2 : How to provide laser beam Wave length (=1m or =10m ) staking cavity or non stacking cavity Choice 3 : e+ stacking in DR or Not
Proof-of-Principle demonstration was done.ATF-Compton Collaboration
Polarized e+ generation: T. Omori et al., PRL 96 (2006) 114801
Polarized -ray generation: M. Fukuda et al., PRL 91(2003)164801