hiroyuki sekiya nnn10 dec 15 2010@toyama hiroyuki sekiya icrr, university of tokyo special thanks t....
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Hiroyuki SekiyaICRR, University of Tokyo
Special Thanks T. Abe
F. Tokanai, & T. SumiyoshiHamamatsu Photonics
Review of photo-sensor R&D for future water Cherenkov
detectorsNNN10 Dec 15 2010
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Contents/Disclaimer
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Many activities aiming for larger/lower cost/mass-production
Quick review of only below technologies◦Super Bi-Alkali /Ultra Bi-Alkali◦Hybrid Photo-Detector◦Gas Photo-Multiplier◦Micro-PMT
Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Do we need R&D?
R3600-05 (The 20 inch PMT) is excellent. It provided reliable detectors and actual results.
To keep the production quality of R3600-05, continues order to Hamamatsu is the best way.
We had better order 100,000 R3600-05s as soon as possible in order to get next generation water Cherenkov detectors within several years.
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Why do we R&D?
Because we want better photon sensors with lower price in short delivery date!
The key motivation is COST.◦Some strategies to reduce cost
Fewer detector with better QE Larger photo-coverage with cheaper sensors Simple structure for short time/mass production etc.
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Pessimistic conclusion
Largest sensors cannot be applied to commercial market. Hamamatsu knows…
Novel prize does not help their sales. Hamamatsu knows…
After all, R3600-05 did not bring so much benefits to Hamamatsu.
If we develop new sensors with them, cost/area may not decrease. It’s completely up to them.
However, actually, they are always willing to develop new sensors with us and they are excellent.
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Super Bi-Alkali/Ultra Bi-Alkali
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Quantum efficiency
Definition: SBA/UBA
ν: frequency of the photon R: reflection coefficientk: total absorption coefficientPν: excitation probability to vacuum levelL: average deviating distance of the excited e-
Ps: extraction probability from the surface
vacuum level
work function
Fermi level
valence band
band gap
electron affinity
γ:hν
Reflection loss Loss in the PC
Excitation efficiency
Extraction efficiency
SBA : reduction of the losses UBA : enhancement of the efficiencies
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
5’’ SBA PMT is available →
So far, UBA is available only for metal package PMTs“transfer” technology is required.
◦ PC is made separately from the tube and assembled
Not cheaper at all.
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Hybrid Photo-Detector(HPD)
Hybrid car◦Ex) Engine + Motor
Hybrid photo sensor◦Ex) Photo tube + Semiconductor
Hybrid gain: Bombardment + Avalanche
TOYOTA PRIUS
Hamamatsu HPDAPD
13’’ HPD
Photo tube (cathode)
Engine
motor
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
HPD -operation principle-PMT
Dynode
APD
×107
× 4500@20kV
Total hybrid gain
×105
× 30
HPD
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Concern? APD high dark current?
P.E. collection efficiencyreaches more than 95%(PMT: 70%)
20kV too high voltage?
No increase in dark current after 1000h operation at 4mARadiation hard.
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Better than PMTs
This implies HPD is not cheaper than PMT.We should not require everything to realize low cost??
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
More Hybrid may reduce total cost
HPD+Electronics(A/D)+HV
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Performance of the Hybrid HPD
Analogue output
1 p.e.
2 p.e.
0 p.e.
1p.e.
2 p.e.
3 p.e.?
Digital output
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
8’’ and 13’’ HPDs available in 2012
Hamamatsu will release in 2012
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Gas Photo-Multiplier(GPM) A kind of Hybrid detectorsElectron multiplication by gaseous avalanche. If combined with photocathode, very large flat-panel
detectors can be realized with much lower cost/area.A weak point → Strategy of “Do not require everything”
F. SauliMichigan University, Ann Arbor - May 23, 2002
LARGE MWPC
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
GPM –operation principle-Photocathode + Micro Pattern Gas Detectors
Combination of MPGDsMulti-stage amplification
Gas avalanche
Total gain ×105
REFLECTIVE PC
TRANSMISSIVE PC
High resolution imaging Possible High QE
photocathode
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Large Area MPGDsVery active R&D and actually in use!
100cmx30cm@CERN
Mesh
Rui de OliveiraMPGD2009
Micromegas with readout Kapton-GEM foil
150cmx50cmfor T2K? TPC
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Large Area MPGDs in JapanVery active R&D and actually in use!
μ-PIC with readout LCP-GEM foil
30cmx30cmfor NEWAGE(Dark Matter Search)
31cmx28cm@Kyoto
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
MPGD2011 will be held in Kobe Aug 29 – Sep 1 2011
2nd International workshop on MPGD followed by RD51 collaboration meeting
Followed by RD51 collaboration meeting (Non-EU hosts for the first time) International organizing committee: A.Cardini (INFN Cagliari), K.Desch (U.Bonn), Th Geralis (Demokritos Athens), I.Giomataris (CEA Saclay), T.Kawamoto (ICEPP Tokyo), A.Ochi (Kobe Univ), V.Polychronakos (BNL), A.Sharma (CERN), S.Uno (KEK), A.White (U.Texas Arlington), J.Wotschack (CERN), Z.Zhao (USTC China)Local organizing committee: J.Haba (KEK), H.Hamagaki (CNS), T.Kawamoto (ICEPP), A.Ochi (Kobe Univ.), H.Sekiya (ICRR), A.Sugiyama (Saga Univ.), A.Taketani (RIKEN), T.Tamagawa (RIKEN), T.Tanimori (Kyoto Univ.), S.Uno (KEK)
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Feedback Problems in photon detection
Ion and photon feedbacks
Limit the stable high gain operation Many activities to overcome the feedbacks.
◦ Gating◦ Ion defocusing by MHSP/COBRA
A.Breskin TIPP09@Tsukuba
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◦ Blind reflection
A. Breskin et al.,T. Sumiyoshiet al.,
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
2GEMs+μPIC with CsI PC 10cm x 10cmPossibility without HamamatsuSo far, tested with UV sensitive CsI
◦ Low Ion feedback achieved!
10cm
Sekiya et al
Anode current
PC current
Deuteron Lump
Ion Back Flow = Ic/Ia < 10-3
@ gas gain 105
54mm
TRANSMISSIVE CsI PC on MgF2 window
REFLECTIVE CsI PCon Au coated LCP-GEM
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
ImagingWith solid UV scintillatorsCan be applied to LAr/LXe
Star
犬
JINST 4 (2009) P11006NIM (2010) doi:10.1016/j.nima.2010.06.114
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Hamamatsu’s GPM
Bialkali PC + glass GEM(capillary plate)
Prototype for R&D
Pyrex glass GEM
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama TIPP09 in Tsukuba 2525
Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
QE in gas is lower –The weak point-
Ne+CF4 gas: 14%( Max @ 350nm)Ar+CF4 gas :12% ( Max @ 420nm)
In vacuum ~ 20%In Ar+CF4 ~ 12%
After evacuation, QE recovered to ~20%.
Trans-missive Photocathode
QE~12%
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Long term stabilityQE maintains almost the same value after 581
days operations.
Period (days)
Rel
ativ
e g
ain
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Strong for Magnetic fieldCompensation coil for terrestrial B free!
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Make it larger Hamamatsu established the production of large
Pyrex grass GEM
thickness 300 mm
diameter at entrance 160 mm
diameter at center 124 mm
pitch 300 mm
Made by a new production Method: Sandblasting
10cm
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
By 2012, they will conclude
Towards large flat panel photo-sensor
100mm square Pyrex glass GEM compared with H8500D
These are assembled in a ceramic vessel?
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
μ-PMT If we don’t require the largeness
Real low cost with real mass-production! MEMS(Micro Electro Mechanical Systems) technology
realized μ-PMT → PMT? , silicon detector? No assemble, completely automated process
Glass base
Silicon base
Glass base(window)
Dynode by micro etching technology
13mm
10mm
Photo cathode(SBA)
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
μ-PMTPrototype: 300 pieces on a 6’’ waferVery uniform quality20% Photo coverage possibility in future??
2x2 sample
Typical output signalof prototype
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Hiroyuki Sekiya NNN10 Dec 15 2010@Toyama
Conclusion
There are many activities that can be applied to next generation large water Cherenkov detector.
Hybrid is also trend in photo-sensors.◦ The 20’’ PMT is still the candidate.◦ SBA technology is already taken into new photo-
sensors.◦ HPD is the most plausible next generation candidate.◦ GPM can be a dark horse. ◦ Post-next generation large sensor?
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