Development of TOP counter for Super B factory K. Inami (Nagoya university) 2007/10/15-20 6 th International Workshop on Ring Imaging Cherenkov Counters.

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Presentation transcript:

Development of TOP counter for Super B factory K. Inami (Nagoya university) 2007/10/ th International Workshop on Ring Imaging Cherenkov Counters - Introduction - Design study - PMT property - Focusing system - Summary

2007/10/15-20 RICH07 2 Side view of Super Belle detector 2.6m 1.2m e - 8.0GeV e + 3.5GeV 1.5T Introduction TOP (Time Of Propagation) counter Developing to upgrade the barrel PID detector For Super B factory L peak ~10 35~36 /cm 2 /s, 20~100 times higher than present Need to work with high beam BG To improve K/  separation power Physics analysis B   /K , , K etc. Flavor tag Full reconstruction Target; 4  for 4 GeV/c

2007/10/15-20 RICH07 3 TOP counter Cherenkov ring in quartz bar Reconstruct ring image using ~20 photons on the screen reflected inside the quartz radiator as a DIRC. Photons are detected with photon detectors. Different ring image for the pion and kaon of the same momentum Need large screen...

2007/10/15-20 RICH07 4 TOP counter 2D position information  Position+Time Compact detector! Linear array PMT (~5mm) Time resolution  ~40ps ~2m KK Simulation 2GeV/c,  =90 deg. ~200ps Different opening angle for the same momentum  Different propagation length(= propagation time) + TOF from IP works additively.

2007/10/15-20 RICH07 5 Test counter Beam KEK PS  2 line 3 GeV/c   beam  in =  in =90 degree Clear ring image Reasonable time resolution Enough bar quality 1mm pitch readout

2007/10/15-20 RICH07 6 Design Quartz: 255cm L x 40cm W x 2cm T Cut at 47.8deg. to reduce chromatic dispersion Multi-anode MCP-PMT Good time resolution (<~40ps), Linear array (5mm pitch) Three readout planes MCP-PMT

2007/10/15-20 RICH07 7 Chromaticity Detection time depending on the wavelength of Cherenkov photons Worse time resolution  Worse ring-image separation  Propagation velocity depending on in the quartz bar

2007/10/15-20 RICH07 8 Chromatic dispersion GaAsP photo-cathode (  alkali p.c.) Higher quantum-efficiency at longer wavelength → less chromatic error Light propagation velocity inside quartz Photon sensitivity at longer wavelength shows the smaller velocity fluctuation. Variation of propagation velocity depending on the wavelength of Cherenkov photons

2007/10/15-20 RICH07 9 GaAsP MCP-PMT development Square-shape MCP-PMT with GaAsP photo-cathode is developed with Hamamatsu Photonics. Prototype GaAsP photo-cathode Al protection layer 2 MCP layers  10  m hole 4ch anodes Slightly large structure Less effective area Performance test Time resolution Target structure

2007/10/15-20 RICH07 10 Wave form, ADC and TDC distributions for single photon Enough gain to detect single photo-electron Good time resolution (TTS=35ps) for single p.e. GaAsP MCP-PMT performance Single p.e. 0.5ns/div 20mV/div pedestal single photon peak Gain ~ 0.64×10 6 TTS~35ps

2007/10/15-20 RICH07 11 Performance with GaAsP K/  separation power GaAsP photo-cathode + >400  m filter, CE=36% 3.5  K/  for 4 GeV/c,  =70 ゚

2007/10/15-20 RICH07 12 Focusing TOP Remaining chromatic effect makes ~100ps fluctuation for TOP. Use dependence of Cherenkov angle to correct chromaticity  Focusing system to measure  c   c  y position Reconstruct ring image from 3D information (time, x and y). Focus Mirror Rotate PMT Side view Mirror image

2007/10/15-20 RICH07 13 Focusing TOP (2)  c ~1.2mrad over sensitive range   y~20mm (~quartz thickness) We can measure dependence and obtain good separation even with narrow mirror and readout plane, because of long propagation length. Not need focusing block Not need fine readout channels 1850mm Virtual readout screen 22mm x 5mm matrix Focusing mirror  c ~1.2mrad

2007/10/15-20 RICH07 14 Performance of focusing TOP K/  separation power GaAsP photo-cathode(+>400  m filter), CE=36% 4.3  separation for 4GeV/c

2007/10/15-20 RICH07 15 Mirror test Prototype by Okamoto-optics 40x2x2cm, R=5m Attached at the end of quartz bar Shape measurement Need continuous mirror image Found (4.9±0.2)mm shift  Adjusted by re-polishing flat planes Focusing mirror 2cm 40cm Spherical mirror (R=5m) Laser depth meter

2007/10/15-20 RICH07 16 Summary R&D of TOP counter is in progress! To install super B factory Design studies To suppress the influence of chromaticity GaAsP photo-cathode MCP-PMT Prototype shows the enough performance Gain = 0.64x10 6, TTS = 35ps for single photon High Q.E. (>40% at 500nm) Focusing system Narrow mirror and narrow readout plane Form large virtual readout screen Not need focusing block and fine PMT channels Improved performance (4.3  for 4GeV/c)  Prototype production