Difference between revisions of "Pion Meeting January 29 2021 11AM ET"
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− | # Lucite detector shielding from downstream and at inner radius (Elham) | + | # Lucite detector shielding from downstream and at inner radius (Elham) [https://moller.jlab.org/cgi-bin/DocDB/private/ShowDocument?docid=687] |
=Attendance= | =Attendance= | ||
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+ | Elham, Wouter, David, Jim | ||
=Minutes= | =Minutes= | ||
+ | |||
+ | * Lucite detector shielding from downstream and at inner radius | ||
+ | ** 3 geometries: "original" with lucite far downstream of Pb donut, "new" with thinner/shorter lucite just downstream of Pb donut, "shielded new" with additional shielding | ||
+ | ** "new" geometry avoids showermax secondaries into lucite in other sector | ||
+ | ** However, still only 10% of light is from Moller electron generator, while there are still 100 times more pions | ||
+ | ** Possible ideas are both low energy electrons and the optical geometry selecting for the backgrounds over forward going pions | ||
+ | ** "shielded new" removes low energy particles that are hitting the lucite when moving backwards | ||
+ | ** Q: What happens if we change the air to vacuum again? How much does scattering of air direct secondaries from the showermax back into the top of lucite detector? | ||
+ | ** Q: How many primary electrons still reach the lucite? Is there punchthrough? | ||
+ | ** Q: Can we replace the donut by a wall with a hole in simulation? | ||
+ | ** Q: Canonical thickness of downstream inner radial lead shielding would be 4". Can this be increased? | ||
+ | ** Q: Diffuse reflection on the lucite surfaces? Fermilab approach. |
Latest revision as of 16:58, 29 January 2021
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Agenda
- Lucite detector shielding from downstream and at inner radius (Elham) [1]
Attendance
Elham, Wouter, David, Jim
Minutes
- Lucite detector shielding from downstream and at inner radius
- 3 geometries: "original" with lucite far downstream of Pb donut, "new" with thinner/shorter lucite just downstream of Pb donut, "shielded new" with additional shielding
- "new" geometry avoids showermax secondaries into lucite in other sector
- However, still only 10% of light is from Moller electron generator, while there are still 100 times more pions
- Possible ideas are both low energy electrons and the optical geometry selecting for the backgrounds over forward going pions
- "shielded new" removes low energy particles that are hitting the lucite when moving backwards
- Q: What happens if we change the air to vacuum again? How much does scattering of air direct secondaries from the showermax back into the top of lucite detector?
- Q: How many primary electrons still reach the lucite? Is there punchthrough?
- Q: Can we replace the donut by a wall with a hole in simulation?
- Q: Canonical thickness of downstream inner radial lead shielding would be 4". Can this be increased?
- Q: Diffuse reflection on the lucite surfaces? Fermilab approach.