emittance growth from elliptical beams and offset collision at lhc and lrbb at rhic ji qiang us larp...
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![Page 1: Emittance Growth from Elliptical Beams and Offset Collision at LHC and LRBB at RHIC Ji Qiang US LARP Workshop, Berkeley, April 26-28, 2006](https://reader030.vdocument.in/reader030/viewer/2022032414/56649ef05503460f94c002c5/html5/thumbnails/1.jpg)
Emittance Growth from Elliptical Beams and Offset Collision at
LHC and LRBB at RHIC
Ji Qiang
US LARP Workshop, Berkeley, April 26-28, 2006
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Outline
• Strong-strong simulation of elliptical colliding beams at LHC
• Offset beam-beam interactions at LHC• Long-range beam-beam effects at RHIC
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Elliptical colliding beams at LHC
• Using Dipole first with doublet focusing• Focuing is symmetric about the IP• Less magnets and lower nonlinear fields at IP• Increase of luminosity
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Computational Model
• Two collision points (no parasitic collisions)
• With 0.212 mrad half crossing angle
• Linear transfer map between IPs
• Tunes (0.31, 0.32)
• Beta* (0.25, 0.25) vs. (0.462,0.135)
• One million macroparticles for each beam
• 128 x 128 x 1 for strong-strong beam-beam force calculation
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RMS Emittance Growth with Round and Elliptical Colliding Beams at LHC
X elliptical
Y elliptical
Y roundX round
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Offset Beam-Beam Collisions at LHC
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Beam energy (TeV) 7
LHC Physical Parameters for the Beam-Beam Simulations
Protons per bunch 10.5e10
* (m) 0.5
Rms spot size (mm) 0.016
Betatron tunes (0.31,0.32)
Rms bunch length (m) 0.077
Synchrotron tune 0.0021
Momentum spread 0.111e-3
Beam-Beam Parameter 0.0034
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IP1
IP5
AB
C D E
F1
2
3 4
5
6
A Schematic Plot of LHC Collision Scheme
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One Turn Transfer Map
M = Ma M1 Mb M2 Mc M3 Md M4 Me M5 Mf M6
M = M6-1 Mf M6 Ma M1 Mb M1-1 M1 M2 M3 M3-1 Mc M3 Md M4 Me M4-1 M4 M5 M6
Here, Ma and Md are the transfer maps from head-on beam-beam collisions; Mb,c,e,f are maps from long-range beam-beam collisions; M1-6 are maps between collision points.
• Linear half ring transfer matrix with phase advanced:
• 90 degree phase advance between long-range collision
points and IPs• 15 parasitic collisions lumped at each long-range
collision point with 9.5 separation
p
66.292;655.312x y
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RMS Emittance Growth vs. Horizontal Separation at LHC(No Parasitic Collisions)
0
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0
RMS Emittance Growth vs. Horizontal Separation at LHC(With 60 lumped Parasitic Collisions)
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Long-Range Beam-Beam Effects at RHIC
• Study the effects of long-range beam-beam (LRBB) at RHIC for the coming wire compensation experiment and find the maximum signal-to-noise ratio setting subject to some limits
• The effects of LRBB subject to • Separation• Tunes• Chromaticity• Sextupole nonlinearity• etc
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Beam energy (GeV) 100
RHIC Physical Parameters
Protons per bunch 2e11
* (m) 1
Transverse Emittance [ mm-mrad] 15
Rms bunch length (m) 0.7
Tunes case 1 (28.68,29.69) and (28.73,29.72)
Momentum spread 0.3e-3
Tunes case 2 (28.68,29.69) and (28.68,29.69)Tunes case 3 (28.73,29.72) and (28.73,29.72)
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Computational Model
•4 x 4 linear transfer map (146 linear map between sextupole)
•Sextupole nonlinearity (144 thin lens kicks)
•Self-consistent strong-strong beam-beam
•1 Million macroparticle for each beam
•128 x 128 x 1 mesh grid
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Averaged Emittance Growth Rate vs. Vertical Separation
Case 3
Case 2
Case 1
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Vertical Emittance Growth without/with Chromaticity
With 6x6 linear map
With 6x6 linear map + chromaticity kick
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Vertical Emittance Growth without/with Sextupoles
With 6x6 linear map
With 4x4 linear map + sextupoles
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Summary
• Initial simulations indicate larger emittance growth from the elliptical colliding beams than the round colliding beams at LHC
• The effects of static offset beam-beam collisions on emittance growth is weak without parasitic collisions at LHC. It can be large with the including of parasitic collisions.
• LRBB at RHIC— Significant emittance growth for beam-beam separation below 4
sigmas— Emittance growth show some dependent on the machine tunes.
For some tunes, the emittance growth shows a linear dependent on separations; Other shows nonlinear dependence. However, beyond 6 sigmas, the emittance growth is no longer sensitive to the machine tunes.
— The effects of chromaticity depends on the machine tunes and becomes weaker for larger separation.
— Stronger sextupole strength might help to improve the signal-to-noise ratio at large separation.
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Future Studies
• Study of emittance growth including parasitic collisions and nonlinear longitudinal map
• Study of emittance using an updated LHC lattice parameters with distributed parasitic collision model
• LRBB at RHIC— Including both chromaticity + sextupole + LRBB in the simulation— Systematic comparison with experiment data— Wire compensation