emittance growth of pb - ions at 17 gev
DESCRIPTION
Emittance growth of Pb - ions at 17 GeV. K. Cornelis, S. Cettour-Cave, J. Ridewood. Why are Ions so different?. Lead ionsProtons. Emittance behaviour at 17 GeV. Intensity 3.5 E10 charges per bunch. Suspected parameters. Space charge. (0.13,0.2). Intrabeam scattering. - PowerPoint PPT PresentationTRANSCRIPT
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Emittance growth of Pb-ions at 17 GeV.
K. Cornelis, S. Cettour-Cave, J. Ridewood
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Why are Ions so different?
Lead ions Protons
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Emittance behaviour at 17 GeV
0 5000 10000 15000 20000 25000 30000 35000 40000 450000
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
Emittance on LHCION flat bottom (NO RF)
HV
Time (ms)
emitt
ance
micr
o m
eter
0 5000 10000150002000025000300003500040000450000
0.5
1
1.5
2
2.5
3
3.5
4
Emittance on LHCION flat bottom (NO RF)
HV
Time (ms)
emitt
ance
micr
o m
eter
Intensity 3.5 E10 charges per bunch
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Suspected parameters
Space charge
Intrabeam scatteringX horrible integrals depending
a.o. on optics.
(0.13,0.2)
Space charge plays certainly a role (no freedom for vertical tune), but what is the impact of IBS ?
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IBS : how it works ?
• A particle that moves forward through the bunch gets knocked by the particles on its way. On the average it gives away momentum, but it also sometimes gains momentum from particles going faster.
• The particles that moves backwards get mainly hit in the back (increased momentum) but sometimes are knocked back by even slower particles.
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IBS : longitudinal phase space
Below transition
Faster
Slower
t
Dp
Faster
Slower
t
Dp
above transition
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IBS
• Below transition the longitudinal motion behaves like a damped oscillator with noise.
• The result will be an Gaussian equilibrium shape. • Important : any particle can move anywhere in the amplitude
distribution. Losses will keep on occurring.• The speed at which the equilibrium is attained and by which
the particles scan different oscillation amplitudes depends on the bunch density.
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IBS in Horizontal plane.
• Random momentum kicks in dispersion regions result in random horizontal kicks giving horizontal blow up.
• There is no damping but the phenomena will slow down as the bunch density is lowering.
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Comparison Q20 and Q26
05000
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2000025000
3000035000
4000045000
0
1
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Emittance growth on FT cycle (Q26)
H20V20H26(2)V26(2)
Time (ms)
Emitt
ance
(micr
omet
er)
0 5000 10000 15000 20000 25000 30000 35000 40000 450000
1
2
3
4
5
6
Emittance growth on FT cycle (Q26)
H20V20H(3)V(3)
TimeEm
ittan
ce (m
icrom
eter
)
-For Q26 optics, emittance growth mainly in horizontal plane
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Horizontal beam profiles
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SUMMARY
• Transverse emittances of Lead Ions are growing at 17GeV.
• Growth rates vary from 10-1 s-1 to 20-1 s-1
• Horizontal blow more important on FT cycle • Hints for IBS contribution.