FLUKA status and plan Sixth TLEP workshop CERN, 16 -18 October 2013
Polarization Wigglers for TLEP and Lessons from LEP
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Transcript of Polarization Wigglers for TLEP and Lessons from LEP
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Polarization Wigglers for TLEP and Lessons from LEP
John Jowett
A quick look at some aspects of the TLEP optics and the wigglers that have also been considered by others (A. Blondel, …).
Apologies that I did no work on TLEP until yesterday.
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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TLEP optics• TLEP optics (80 km)
from Bernhard Holzer used in following
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
Arc cell
At first I thought the quadrupoles were too short for good damping aperture.
IR1
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TLEP parameter lists and emittance
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
Must to do something to create much larger emittance at lower energies.
Natural emittance of TLEP lattice
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Alain Blondel 5th TLEP workshop 2013-07-25
optics – TLEP arc cell
r=3100 m, Lcell=79 m r=9100 m, Lcell=50 m
Y. Cai, B. Holzer, H. Burkhardt
ex=48 nm at 104.5 GeV → ex=1.5 nm at 175 GeV
from LEP to TLEP
beta functionsdispersion
𝜀∝𝛾2𝜃❑3: at lower beam energy increase cell length (“q”) x2 or x6!
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Emittance control at lower energies
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
This will give >500 m in arc cells 300 m long.
What are the aperture requirements?
Can the dispersion still be matched with the same dispersion suppressors? Of course one can also play with Jx and reduce the phase advance but this is a big factor.
Stop Press: since Bernhard’s talk, I evaluated the vertical emittance from the opening angle of synchrotron radiation: 1.5 am
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Damping aperture
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
2
FODOFODO F
2 532
2
8
2
2 28 1
ODO
2
5532 3
4, 2 2 , =1
Synchrotron integrals are well known,
81 9 cos csc2
200
Damping apert
e
ure limit is
xcept m
r
aybe
eache
x exe
y e
xQ
x y
Ic EJ Im c
IJ J J J JI
I K D dsL
IL
e e
e
8
2
or becomes zero.
In TLEP lattice ' 2 219 damping aperture 1.3% in .
With 6 longer cells, this will be reduced to 0.2% in possible concern? May be very di
d when
fficult
either x
e
e
J J
IJI
e
e
to find an initial damped closed orbit.
Solution may be to lengthen quadrupoles and or reduce betatron phase advance.
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History of the wigglers in LEP• In 1983 we proposed an installation of 16 asymmetric
wigglers in LEP to control emittance (luminosity at beam-beam limit), increase radiation damping and enhance the Sokolov-Ternov polarization rate.
• At the time, polarization was considered a chimera (plus ça change …) and money was scarce, so we got only 8 wigglers, enough to serve the first two purposes reasonably well.
• There were then 2 families of wigglers in the LEP design:– The 4 Emittance Wigglers, located in missing-dipole space in
the dispersion suppressors where Dx>0. – The 4 Damping Wigglers, located in matching sections where
Dx=0. J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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LEP Emittance and Damping Wigglers
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
http://accelconf.web.cern.ch/AccelConf/p83/PDF/PAC1983_2581.PDF
Well-thought out integral magnet design
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Ideal polarization performance of LEP E- and D-wigglers
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
We nevertheless managed to include a moderate asymmetry parameter (2.5) so that the polarization would have a chance.
We did all this shortly before the Z-boson, the particle of the moment, was discovered at a relatively low mass (plus ça change …) and when there was little quantitative information on depolarization effects.
This plot shows the wiggler field necessary to keep emittance constant.
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Wiggler compensation
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
Integral magnet design, Field integral well cancelled by built-in trims.
Wigglers excitations were the only non-linear knobs in LEP. Wiggler field was accompanied by approximately quadratic shifts in nearby quadrupole strengths designed to match out tune changes from weak-focusing in wiggler dipoles. Worked perfectly from theory.
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11J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
• By 1988, the prospect of longitudinally polarized e+e- collisions at the Z-pole was taken seriously thanks, in particular, to the advocacy of Alain Blondel (plus ça change …) who stressed the need for faster polarization.
• Hence more, stronger wigglers …
http://cds.cern.ch/record/442913
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Concept for Polarization Wigglers in LEP
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
http://accelconf.web.cern.ch/AccelConf/e92/PDF/EPAC1992_0649.PDF
Innovative (=cheap, quick) magnet design. Left-over LEP concrete dipoles were sawn in half to make the weak outer poles. Separate short dipole for strong centre pole.
Operationally very troublesome orbit effects despite special trim coils. Large energy spread and betatron tune spread. EPAC
1992
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Parameters, vacuum effects
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
Had to remove collimators away from wigglers.Later, the radiation from these wigglers caused significant damage to vacuum chambers.
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Benefits of the Polarization Wigglers in LEP• As polarization levels were relatively low (but enough
for energy calibration ), the effective growth time of transverse polarization was acceptable and wigglers were not needed at 46 GeV.
• Bunch-lengthening and enhanced damping at injection mitigated the Transverse Mode-Coupling Instability (TMCI), allowed record single-bunch currents, raising luminosity for LEP2.
• Spin-rotators were never installed … if you ever want them, make sure they are NOT AN AFTERTHOUGHT, but worked into the basic design of the interaction regions.
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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Wigglers and radiation integrals
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
B
/B B r
L rL
/B B r /B B r
L rL L rLL
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Emittance, energy spread
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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Faster polarization increases energy spread
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
Once the energy spread becomes comparable with 440 MeV, the spacing between the integer spin resonances, strong depolarization occurs.
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Polarization level
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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Low polarization level is “better”
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
1 1 1eff
In the presence of depolarizing effects, the asymptotic level is
8 11 /5 3
and the effective polarization time is given by
p d
p p d
P
Go to CDF file …
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12 wigglers flat-out, ideal polarization
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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Possible solution, reduced field, 3 wigglers
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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Residual dispersion at wiggler
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
Ideal Dispersion error
May increase emittance a bit (not a problem).
May also depolarize/complicate spin-matching of wigglers.
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Conclusions• The FODO cell design of the TLEP arcs may need longer
quadrupoles to allow operation at Z energy. – Might also need to review dispersion suppressors?
• Wigglers can be used to enhance polarization rate but the available parameter space is very limited (low polarization levels, moderate wiggler fields and lengths).
• Huge flux of synchrotron radiation from wigglers.• Emittance wigglers might be useful, if so leave some missing
dipoles in Dispersion suppressors.
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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BACKUP SLIDES
J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013
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25J.M. Jowett,6th TLEP Workshop, CERN 16/10/2013