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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 Status report of offset and angle studies with Guinea-Pig Status report of offset and angle studies with Guinea-Pig Isabell-Alissandra Melzer-Pellmann ILC tech meeting July 11 th, 2006
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 2 Offset and angle scan from 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 from beam-beam simulation with GUINEA-PIG from TESLA TDR
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 3 Offset scan with ILC parameters ILC parameters: ILC 500 NOM: y = 5.7nm ILC 500 LOW Q: y = 3.5nm ILC 500 LARGE Y: y = 8.1nm ILC 500 LOW P: y = 3.8nm ILC 500 HIGH L: y = 3.5nm ILC 1000 NOM: y = 3.5nm ILC 1000 LOW Q: y = 2.5nm ILC 1000 LARGE Y: y = 7.0nm ILC 1000 LOW P: y = 2.7nm ILC 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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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 4 Offset scan with ILC parameters ILC parameters: ILC 500 NOM: y = 5.7nm ILC 500 LOW Q: y = 3.5nm ILC 500 LARGE Y: y = 8.1nm ILC 500 LOW P: y = 3.8nm ILC 1000 NOM: y = 3.5nm ILC 1000 LOW Q: y = 2.5nm ILC 1000 LARGE Y: y = 7.0nm ILC 1000 LOW P: y = 2.7nm Loss of luminosity falls not so steep, for y/ y =±1 O(30%) (TESLA: for y/ y =±1 O(40%))
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 5 Angle scan with ILC parameters ILC parameters: ILC 500 NOM: y = 14.3 rad ILC 500 LOW Q: y = 17.5 rad ILC 500 LARGE Y: y = 20.2 rad ILC 500 LOW P: y = 18.9 rad ILC 500 HIGH L: y = 17.5 rad ILC 1000 NOM: y = 11.7 rad ILC 1000 LOW Q: y = 12.4 rad ILC 1000 LARGE Y: y = 11.7 rad ILC 1000 LOW P: y = 13.4 rad ILC 1000 HIGH L: y = 12.4 rad Changing variable angle_y in Guinea-Pig results in almost no change (tested also with TESLA parameters) - contacted Daniel Schulte… waiting for response
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 6 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 from beam-beam simulation with GUINEA-PIG from TESLA TDR
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 7 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) Status: generated beam (without change yet) fed into Guinea-Pig, compared beam generated by Guinea-Pig with my generated beam after interaction (output from Guinea-Pig) - see next pages differences observed need to check this before further simulation can be run. wrong calculation of x’, y’? x/ m y/ m z/ m
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 8 Comparison: Guinea Pig generated beam vs my generated beam (after interaction) Guinea-Pig generated With root random number generator generated beam. z/ m x/ m y/ m z/ m y/ m x/ m
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 9 Comparison: Guinea Pig generated beam vs my generated beam (after interaction) Guinea-Pig generated With root random number generator generated beam. x/ m y/ m
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 10 Comparison: Guinea Pig generated beam vs my generated beam (after interaction) Guinea-Pig generated With root random number generator generated beam. x/ m z/ m z-distribution seems ok x-distribution seems ok exept around 0
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Isabell-A. Melzer-Pellmann ILC-tech meeting, 24.8.2006 11 Comparison: Guinea Pig generated beam vs my generated beam (after interaction) Guinea-Pig generated With root random number generator generated beam. z/ m y/ m y-distribution has large tails
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