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Electron mode A B C D > 4 GeV e- θ g e- DR α PS

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Presentation on theme: "Electron mode A B C D > 4 GeV e- θ g e- DR α PS"— Presentation transcript:

1 Electron mode A B C D > 4 GeV e- θ g e- DR α PS
GUN SHB L GeV 5.7 GeV 0.1GeV 0.8 GeV ≈ 70 m. ≈ 320 m. PS ≈ 60 m. Linac B turned down to 2.7 GeV. Low charge e bunches injected in DR with the pulsed a and, the same time, damped e bunches are extracted with the pulsed g and accelerated to 4 GeV. 3) e bunches pass off-axis (≈ 1mm), through a target hole. Legend e low charge electron bunches p positron bunches E high charge electron bunches

2 Positron mode A B C D θ > 7 GeV e+ β PS e+ DR
GUN SHB L GeV 5.7 GeV 0.1GeV 0.8 GeV > 7 GeV e+ ≈ 70 m. PS ≈ 60 m. ≈ 320 m. e+ DR ≈ 400 m. 1) Linac B turned up to 5.7 GeV. 2) Linac C is aligned with emerging, low-energy p. 3) Dampep p bunches are extracted from pDR, injected in the linac with the DC dipole b and accelerated along linacs B-C-D, up to 7 GeV. The p bunches pass through a target hole. 4) Dampep p bunches may not be extracted after the arrival of the recirculated p’s because the RF sections, meanwhile, are switched-off. 5) High charge E- bunches are generated about 70 nsec behind the p bunches and accelerated by linac A. 6) E- bunches are injected in the linac B, with the DC dipole b, are accelerated, together with the p’s, and finally hit the target. 7) Emerging p bunches are accelerated to 0.8 GeV by linacs C-D and recirculated back to the pDR. Legend e low charge electron bunches p positron bunches E high charge electron bunches

3 Linac C Linac B P.S. area close-up view PS new linac axis l d
Pulsed Focusing coil Linac C new linac axis l d Linac B Pulsed dipoles PS Here, a pulsed device must re-position the damped bunches on the center line The PS area concerns the operation of 3 type of bunches: Low charge damped electron bunches: must travel through the PS-hole High charge Electron bunches: must hit the PS bulk. ……Low energy positron bunches follow along a straigth trajectory. Low charge damped positron bunches: must travel through the PS-hole Both e and p damped bunches pass through the same PS-hole, thanks to the pulsed dipoles l and d.

4 A B C D DIPOLES Timing ------ 1) dipole α and g…. on-off @ 50 Hz
2) dipole β and q… DC dipoles 4) dipoles l and d ….. Pulsed inverted 50 Hz e- DR A R B C D θ α β g GUN SHB L GeV 5.7 GeV 0.1GeV 0.8 GeV > 7 GeV e+ ≈ 70 m. ≈ 60 m. ≈ 320 m. PS e+ DR ≈ 400 m.


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