CW 2GeV Linac Error Simulations at 10 mA 80 parameters scanned / New - PowerPoint PPT Presentation

CW 2GeV Linac Error Simulations at 10 mA 80 parameters scanned / ”New TRACK” Jean-Paul Carneiro March 23, 2010

ALIGN Parameter TRACKv39 n ALIGN name δ xy δ z φ z δφ dyn . δ F dyn . δφ static δ F static ◮ From RFQ exit to end of the CW 2 GeV linac ( ∼ 400 meters) ◮ 80 errors simulated with TRACKv39 ◮ Each error simulated with 100 runs with 3D SC (10 mA) ◮ 80 × 100=8000 runs with TRACKv39 on FermiGrid

Parameters 01-20 ◮ 11/ Sol. Field δ F dynamic = 0 . 5 % ◮ 01/ Solenoids δ xy = 150 µ m ◮ 12/ Sol. Field δ F dynamic = 1 . 0 % ◮ 02/ Solenoids δ xy = 300 µ m ◮ 13/ Sol. Field δ F dynamic = 1 . 5 % ◮ 03/ Solenoids δ xy = 500 µ m ◮ 14/ Sol. Field δ F dynamic = 2 . 0 % ◮ 04/ Solenoids δ xy = 750 µ m ◮ 15/ Sol. Field δ F dynamic = 2 . 5 % ◮ 05/ Solenoids δ xy = 1000 µ m ◮ 16/ Sol. Field δ F static = 0 . 5 % ◮ 06/ Solenoids δ z = 150 µ m ◮ 17/ Sol. Field δ F static = 1 . 0 % ◮ 07/ Solenoids δ z = 300 µ m ◮ 18/ Sol. Field δ F static = 1 . 5 % ◮ 08/ Solenoids δ z = 500 µ m ◮ 19/ Sol. Field δ F static = 2 . 0 % ◮ 09/ Solenoids δ z = 750 µ m ◮ 20/ Sol. Field δ F static = 2 . 5 % ◮ 10/ Solenoids δ z = 1000 µ m

Parameters 21-40 ◮ 31/ Quads φ z = 1 mrad ◮ 21/ Quads δ xy = 150 µ m ◮ 32/ Quads φ z = 2 mrad ◮ 22/ Quads δ xy = 300 µ m ◮ 33/ Quads φ z = 5 mrad ◮ 23/ Quads δ xy = 500 µ m ◮ 34/ Quads φ z = 7 mrad ◮ 24/ Quads δ xy = 750 µ m ◮ 35/ Quads φ z = 10 mrad ◮ 25/ Quads δ xy = 1000 µ m ◮ 36/ Quads Field δ F dynamic = 0 . 5 % ◮ 26/ Quads δ z = 150 µ m ◮ 37/ Quads Field δ F dynamic = 1 . 0 % ◮ 27/ Quads δ z = 300 µ m ◮ 38/ Quads Field δ F dynamic = 1 . 5 % ◮ 28/ Quads δ z = 500 µ m ◮ 39/ Quads Field δ F dynamic = 2 . 0 % ◮ 29/ Quads δ z = 750 µ m ◮ 40/ Quads Field δ F dynamic = 2 . 5 % ◮ 30/ Quads δ z = 1000 µ m

Parameters 41-60 ◮ 51/ Cav. δ z = 150 µ m ◮ 41/ Quads Field δ F static = 0 . 5 % ◮ 52/ Cav. δ z = 300 µ m ◮ 42/ Quads Field δ F static = 1 . 0 % ◮ 53/ Cav. δ z = 500 µ m ◮ 43/ Quads Field δ F static = 1 . 5 % ◮ 54/ Cav. δ z = 750 µ m ◮ 44/ Quads Field δ F static = 2 . 0 % ◮ 55/ Cav. δ z = 1000 µ m ◮ 45/ Quads Field δ F static = 2 . 5 % ◮ 56/ Cav. φ z = 1 mrad ◮ 46/ Cav. δ xy = 150 µ m ◮ 57/ Cav. φ z = 2 mrad ◮ 47/ Cav. δ xy = 300 µ m ◮ 58/ Cav. φ z = 5 mrad ◮ 48/ Cav. δ xy = 500 µ m ◮ 59/ Cav. φ z = 7 mrad ◮ 49/ Cav. δ xy = 750 µ m ◮ 60/ Cav. φ z = 10 mrad ◮ 50/ Cav. δ xy = 1000 µ m

Parameters 61-80 ◮ 71/ Cav. Phase δφ static = 0 . 5 ◦ ◮ 61/ Cav. Phase δφ dynamic = 0 . 5 ◦ ◮ 72/ Cav. Phase δφ static = 1 . 0 ◦ ◮ 62/ Cav. Phase δφ dynamic = 1 . 0 ◦ ◮ 73/ Cav. Phase δφ static = 1 . 5 ◦ ◮ 63/ Cav. Phase δφ dynamic = 1 . 5 ◦ ◮ 74/ Cav. Phase δφ static = 2 . 0 ◦ ◮ 64/ Cav. Phase δφ dynamic = 2 . 0 ◦ ◮ 75/ Cav. Phase δφ static = 2 . 5 ◦ ◮ 65/ Cav. Phase δφ dynamic = 2 . 5 ◦ ◮ 76/ Cav. Field δ F static = 0 . 5 % ◮ 66/ Cav. Field δ F dynamic = 0 . 5 % ◮ 77/ Cav. Field δ F static = 1 . 0 % ◮ 67/ Cav. Field δ F dynamic = 1 . 0 % ◮ 78/ Cav. Field δ F static = 1 . 5 % ◮ 68/ Cav. Field δ F dynamic = 1 . 5 % ◮ 79/ Cav. Field δ F static = 2 . 0 % ◮ 69/ Cav. Field δ F dynamic = 2 . 0 % ◮ 80/ Cav. Field δ F static = 2 . 5 % ◮ 70/ Cav. Field δ F dynamic = 2 . 5 %

(181) Solenoids δ xy = 150 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(182) Solenoids δ xy = 300 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(183) Solenoids δ xy = 500 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(184) Solenoids δ xy = 750 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(185) Solenoids δ xy = 1000 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(186) Solenoids δ z = 150 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(187) Solenoids δ z = 300 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance z

(188) Solenoids δ z = 500 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(189) Solenoids δ z = 750 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(190) Solenoids δ z = 1000 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(191) Sol. Field δ F dynamic = 0 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(192) Sol. Field δ F dynamic = 1 . 0 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(193) Sol. Field δ F dynamic = 1 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(194) Sol. Field δ F dynamic = 2 . 0 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(195) Sol. Field δ F dynamic = 2 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(196) Sol. Field δ F static = 0 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(197) Sol. Field δ F static = 1 . 0 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(198) Sol. Field δ F static = 1 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(199) Sol. Field δ F static = 2 . 0 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(200) Sol. Field δ F static = 2 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(201) Quads δ xy = 150 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(202) Quads δ xy = 300 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(203) Quads δ xy = 500 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(204) Quads δ xy = 750 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(205) Quads δ xy = 1000 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(206) Quads δ z = 150 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(207) Quads δ z = 300 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance z

(208) Quads δ z = 500 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(209) Quads δ z = 750 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(210) Quads δ z = 1000 µ m Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(211) Quads φ z = 1 mrad Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(212) Quads φ z = 2 mrad Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(213) Quads φ z = 5 mrad Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(214) Quads φ z = 7 mrad Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(215) Quads φ z = 10 mrad Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(216) Quads Field δ F dynamic = 0 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(217) Quads Field δ F dynamic = 1 . 0 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(218) Quads Field δ F dynamic = 1 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(219) Quads Field δ F dynamic = 2 . 0 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(220) Quads Field δ F dynamic = 2 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(221) Quads Field δ F static = 0 . 5 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z

(222) Quads Field δ F static = 1 . 0 % Figure: RMS Emittance X Figure: RMS Emittance Y Figure: Losses [W · m − 1 ] Figure: RMS Emittance Z