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LTR for ILC e- (eLTR) RF section solenoid section.

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Presentation on theme: "LTR for ILC e- (eLTR) RF section solenoid section."— Presentation transcript:

1 LTR for ILC e- (eLTR) RF section solenoid section

2 Magnet details for eLTR L (m)  B/  x  (T/m) BL (T.m) Radius or half gap (cm) QuantityNOTE Qmat11 Qmat12 Qmat13 Qmat14 Bend1 Bend2 Qarc1 Qarc2 Qarc3 Qarc4 Qmat21 Qmat22 Qmat31 Qmat32 Qmat33 Qmat41 Qmat42 Qmat43 0.2 2 1 0.1 0.2 0.1 0.2 0.1 0.2 8.3 9.5 13.5 7 27.2 26.7 25.5 34 32.8 27 37 25.8 38.8 40.5 19.7 1.92 0.96 111144142111111111111144142111111111 Matching from booster exit to entrance of eLTR (not shown in the 1 st slide) eLTR arc section Matching from arc exit to entrance of RF section Matching from exit of rf section to entrance of solenoid Matching from solenoid section exit to DR entrance

3 Other info for eLTR Total bending angle=5  7.931°; R56 is 50cm at the present settings; R56 is adjustable by changing current of arc quads. 5-6 m space for RF section Another 5-6m for solenoid section (~26.2 T.m)

4 Complete optics of ILC e- injector beamline - Bunching system (120 keV to 11 MeV) with Parmela - Pre-acceleration (11 MeV to 84 MeV) with Parmela - Dogleg - Booster linac (84 MeV to 5 GeV) - eLTR to damping ring All components are connected

5 Two 5-cell SW L-band 108MHz SHB 433 MHz SHB 1 st structure2 nd structure triplet to 84 MeV ILC e- injector: 120 keV to 84 MeV

6 ILC e- injector up to entrance of eLTR (5 GeV)

7 Half size at ILC e- injector up to entrance of eLTR (5 GeV)


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