offset and angle studies with guinea-pig
DESCRIPTION
Offset and angle studies with Guinea-Pig . Isabell-Alissandra Melzer-Pellmann Linear Collider Workshop ILC 2007 May 30 th -June 3 rd , 2007. Offset and angle scan from TESLA TDR. Luminosity drops fast with small change of offset and/or angle. Results from beam-beam simulation with - PowerPoint PPT PresentationTRANSCRIPT
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Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset and angle studies Offset and angle studies with Guinea-Pig with Guinea-Pig
Isabell-Alissandra Melzer-PellmannIsabell-Alissandra Melzer-Pellmann
Linear Collider WorkshopLinear Collider Workshop
ILC 2007ILC 2007
May 30May 30thth-June 3-June 3rdrd, 2007, 2007
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2Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset and angle scanfrom TESLA TDR
Luminosity drops fast with small change of offset and/or angle
TESLA parameters: y = 5nm , y = 12 rad
How is the luminosity change for the ILC parameters?
Results frombeam-beamsimulation with GUINEA-PIGfrom TESLA TDR
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3Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan with ILC parameter set from 2005
ILC parameters: ILC 500 NOM: y = 5.7nmILC 500 LOW Q: y = 3.5nmILC 500 LARGE Y:y = 8.1nmILC 500 LOW P: y = 3.8nmILC 500 HIGH L: y = 3.5nm
ILC 1000 NOM: y = 3.5nmILC 1000 LOW Q: y = 2.5nmILC 1000 LARGE Y:y = 7.0nmILC 1000 LOW P: y = 2.7nmILC 1000 HIGH L: y = 2.5nm
Loss of luminosity falls not so steep,for y/y=±1 O(30%) (TESLA: for y/y=±1 O(40%))
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4Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan with ILC parameters
Line for no beam-beam interaction added:L/Lnom=exp(1/4 ·(y/y)2)
Loss of luminosity falls not so steep,for y/y=±1 O(25%) (TESLA: for y/y=±1 O(40%))
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5Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Angle scan with ILC parameters
ILC parameters: ILC 500 NOM: y = 14.3radILC 500 LOW Q: y = 17.5radILC 500 LARGE Y:y = 20.2radILC 500 LOW P: y = 18.9radILC 500 HIGH L: y = 17.5rad
ILC 1000 NOM: y = 11.7radILC 1000 LOW Q: y = 12.4radILC 1000 LARGE Y:y = 11.7radILC 1000 LOW P: y = 13.4radILC 1000 HIGH L: y = 12.4rad
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6Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Angle scan with ILC parameters
ILC parameters: ILC 500 NOM: y = 14.3radILC 500 LOW Q: y = 17.5radILC 500 LARGE Y:y = 20.2radILC 500 LOW P: y = 18.9radILC 500 HIGH L: y = 17.5rad
ILC 1000 NOM: y = 11.7radILC 1000 LOW Q: y = 12.4radILC 1000 LARGE Y:y = 11.7radILC 1000 LOW P: y = 13.4radILC 1000 HIGH L: y = 12.4rad
Only 10% loss for LOW Q option, largest loss of 40% for LARGE Y option!
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7Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Next step: include ‘banana effect’
Banana effect: internal bunch deformations, induced by single-bunch wakefields in the linac.
TESLA TDR: single bunch correlated emittance growth expected to be 6% in average.
Results frombeam-beamsimulation with GUINEA-PIGfrom TESLA TDR
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8Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Next step: include ‘banana effect’
For these plots a ‘banana shape’ beam needs to be feeded into Guinea-Pig• Simulated ‘banana’ from MERLIN not yet available.• Idea: just generate beam with ILC parameters and change it linearly by average of 6% (number from TESLA TDR)
y/m
z/m
y/m
z/m
Examples: Beam for ILC-NOM-500 Beam for ILC-NOM-500 with 100% correlated emittance growth (to make the effect visible)
0 @ 1z
100% off @ 1Y
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9Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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10Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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11Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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12Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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13Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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14Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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15Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Conclusion
• Offset scan has similar effect for all parameter sets• Angle scan has smallest effect on LOWQ and largest effect on LARGEY parameter sets.
• Effect of wake fields causing banana deformation in beams is less pronounced for the ILC parameters than for the TESLA parameters (so far just tested with linear correlated emittance growth)
• Possibility to get 100% luminosity for all parameter sets when performing an offset scan followed by an angle scan
• TO DO: Feed more realistic banana beam (e.g. output from Merlin when available) into Guinea-Pig
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16Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
BACKUP transparencies
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17Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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18Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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19Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value
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20Isabell-A. Melzer-Pellmann ICL 2007, 30.5.-3.6.2007
Offset scan followed by angle scan for best offset
value