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Calorimeter Transition Region Richard Jones & Paul Eugenio GlueX Collaboration Meeting January 11, 2008.

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Presentation on theme: "Calorimeter Transition Region Richard Jones & Paul Eugenio GlueX Collaboration Meeting January 11, 2008."— Presentation transcript:

1 Calorimeter Transition Region Richard Jones & Paul Eugenio GlueX Collaboration Meeting January 11, 2008

2 Calorimeter Transition Region

3 CD3 geometry improved, but gap still apparent

4 Gap Access via Cerenkov voids Redesigned Cerenkov housing gap access

5 Add Conic Gap Calorimeter

6 Gap Calorimeter 0 17 + 6565 407 48 segment conical unit 9o9o 11 o GCAL 435460 cm

7 GCAL module concept Use BCAL module to construct GCAL modules  machine 16 GCAL per BCAL module  requires 3 additional BCAL modules (48→51, +6%)‏ 25 cm 8 cm 14 cm 10 cm 13 cm GCAL cone

8 Example: 1 GeV photon at 9.3º Provides a clean definition of the forward calorimeter acceptance

9 Noticethe early conversion in the cables is 99% recovered in the GCal Notice: the early conversion in the cables is 99% recovered in the GCal Example: 1 GeV photon at 10º

10 This is clearly the most difficult case. E bcal +E gcal = 88% E0 Notice:in addition to capturing most of the escape energy, the Gcal also shadows the Fcal from the forward splash Notice: in addition to capturing most of the escape energy, the Gcal also shadows the Fcal from the forward splash Example: 1 GeV photon at 11º

11 By 12º the BCal captures the entire shower Example: 1 GeV photon at 12º

12 No clustering, just summing energy but proximity to source means that the energy is highly localized – see event image at 10º These photons are substantially lost in the simulation without the GCal Energy Spectrum: 1 GeV photons at 10.5º


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