Title: Catcher
1Catcher
- Scope of subsystem
- Current specification from physics
- Current design
- Open issues
- Resources
2Scope of subsystem
- Photon veto inside/near the beam at downstream
end - TASK
- Detect photons from KL decays passing through the
beam hole - Be insensitive to a vast amount of unwanted
neutrons - SOLUTION ? Utilize Cherenkov radiation
- Lead and aerogel tile sandwich counter inside the
beam named aerogel catcher - Lead and acrylic slab sandwich counter near the
beam named guard counter
3Specification from physics
- Photon Efficiency
- Energy spectrum of photonswhich go into the
catcher after canonical kinematical cuts(Kp2
dominated by odd pairing events) - gt98 for 300MeV photons
- gt99 for more energetic ones
- Sensitivity to neutrons, KLs
- To avoid false vetoes by beam neutrons and
surviving KLs - lt0.3 for neutrons with Ekin800MeV
- KL decaying in the catcher ends up to be
detected,but false veto probability should be
kept less than a few
4Current design Overview
Guard counter
Aerogel Catcher
beam
5AEROGEL CATCHER Principle of aerogel catcher
- AEROGEL CATCHER
- Lead and aerogel tile counter
- Avoid detection of slow particlesfrom neutron
interactions - Distributed arrangement
- Coincidence along the beamhelps us catch forward
g only
6AEROGEL CATCHER Module - Elements / Optics
- Parameters of each module
- To get more Cherenkov lights
- To simplify optics for easy production
TDR design
Current design
7AEROGEL CATCHER Configuration
- Distributed arrangement
- Module size 30cm x 30cm
- Pb converter 2mmt per layer
- Number of modules 420
- 12-21 in horizontal with beam divergence
- 25 layers along beam(8.3 X0 in total)
- Z gap between layers 35cm
- Coincidence condition
- gt 4 p.e. in 1st layer (A)
- gt 2 p.e. in 2nd layer (B)
Beam envelop
Top view
12m downstream of main detector
8Expected performance of AEROGEL CATCHER Photon
efficiency / Neutron sensitivity
- Average over the whole position and angle
Neutron sensitivity
Photon efficiency
gt99 _at_ 300MeV
0.3 _at_ 0.8GeV
9GUARD COUNTER Principle of guard counter
- GUARD COUNTER
- Lead and acrylic slab counter
- Slow particle doesnt emit Cherenkov light
- Utilize the total reflection angle in light
transportation - Cherenkov lights from slow particlesdont
fulfill the total reflection condition
Photon
Neutron
10Current design of GUARD COUNTER Guard counter
- Counter to cover the halo region
- Soft but many neutrons around the beam
- Lead acrylic slab sandwich
- Size 15cm x 15cm
- 8 layers of 2mm Pb 10mm acrylic
- Read by 5 inch PMT
- 3 modules along the beam
- Number of modules 144
Side View
beam
Front View
Module
11Expected performance of WHOLE CATCHER SYSTEM
Efficiency map of catcher guard counter
12Justification of the conceptual design
Prototypes so far
PT2
- Prototype 1 (2001-2)
- 1/4 size, flat mirror
- light yield
- Prototype 2 (2002-3)
- 1/4 size, parabolic mirror
- light yield
- response to proton (as substitute for neutron)
- Check single layer eff. / two-layers
coincidence - Good agreement with MC(with gas scintillation)
PT1