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Hall A Pressurized Gas Cerenkov Design Goals:  Separate  and K for p>2.3GeV/c.  Continue to differentiate e/  Features:  Operates at pressures up.

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Presentation on theme: "Hall A Pressurized Gas Cerenkov Design Goals:  Separate  and K for p>2.3GeV/c.  Continue to differentiate e/  Features:  Operates at pressures up."— Presentation transcript:

1 Hall A Pressurized Gas Cerenkov Design Goals:  Separate  and K for p>2.3GeV/c.  Continue to differentiate e/  Features:  Operates at pressures up to 10 psig, using C 4 F 10 or CO 2 as the radiator.  Expect average of 10 p.e. for a 2.3GeV/c pion with C 4 F 10   rejection factor of 400 (3 p.e. cutoff) Experiments:Pentaquark (E05-009), Transversity SSA (E03-004), Flavor Asymmetry in SIDIS (PR04-114 cond. app.) Design and fabrication in collaboration with: Argonne National Laboratory, Rutgers University, and Jefferson Lab

2 Design performance

3 Design (cont) Control cost and effort by re-using optics from present cerenkov. Can the present box be re-used? What modifications are necessary? Finite element analysis by Ravi Anumagalla

4 Design performance

5 Model 4: No top and Bottom faces, includes a “C” Channel on one face Max Stress : 263 ksi Max Deflection : 1.59 inches Boundary Conditions: Pressure on all faces (14.7 psi), Fixed at the bottom and top surface,

6 Model 4: Plot shows surfaces where stresses are in the range of 0-23 ksi

7

8 Design (cont) Control cost and effort by re-using optics from present cerenkov. Can the present box be re-used? What modifications are necessary? Finite element analysis by Ravi Anumagalla –Weight goes from 750lbs to ~2200lbs. Another idea by Bogdan: titanium cylinder with interior supports (being priced now)

9 Bogdan’s concept

10 Common features PMT sealed against interior for servicing while the chamber is pressurized. Simple stationary gas system since it will be filled from the Hall B gas system. Size is compatible with current short cerenkov. Low-number of knock-on electrons for 0.4mm Ti window (<2%).

11 0.36%

12 Conclusion Pressurized Cerenkov design continuing. Should provide excellent pi/K separation for momenta greater than 2.3 GeV/c Need to finalize the design (after cost estimates are made)

13 R ich  /K separation for p > 2.5 GeV/c Radiator C6F14 n=1.29  Ch ~ 5mr Radiator C5F12 n=1.24  Ch ~ 5mr 4  separation at ~ 2.5 GeV/c4  separation at ~ 3.0 GeV/c Mauro Iodice – R ICH2004 - Playa del Carmen, Mexico - Nov.30 Dec. 5, 2004

14 R ich  /K separation with C5F12 (n=1.24) radiator (14 cm proximity gap) >20  separation at ~ 2 GeV/c ~ 4  separation at 3.0 GeV/c Mauro Iodice – R ICH2004 - Playa del Carmen, Mexico - Nov.30 Dec. 5, 2004 M onte C arlo Simulations


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