Tests of the BURLE 64-anode MCP PMT as the detector of...
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![Page 1: Tests of the BURLE 64-anode MCP PMT as the detector of ...ndip.in2p3.fr/beaune05/cdrom/Sessions/krizan.pdf · as the detector of Cherenkov photons Peter Križan University of Ljubljana](https://reader031.fdocuments.net/reader031/viewer/2022022011/5b0b45f77f8b9adc138d92f1/html5/thumbnails/1.jpg)
June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Tests of the BURLE 64-anode MCP PMTas the detector of Cherenkov photons
Peter KrižanUniversity of Ljubljana and J. Stefan Institute
![Page 2: Tests of the BURLE 64-anode MCP PMT as the detector of ...ndip.in2p3.fr/beaune05/cdrom/Sessions/krizan.pdf · as the detector of Cherenkov photons Peter Križan University of Ljubljana](https://reader031.fdocuments.net/reader031/viewer/2022022011/5b0b45f77f8b9adc138d92f1/html5/thumbnails/2.jpg)
June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Contents
Motivation and requirements
BURLE MCP-PMT
Beam test results
Bench tests
Summary, outlook
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Belle Spectrometer - PID
Particle identification:●TOF●dE/dx●ACC: threshold aerogel Cherenkov counter
Large solid angle detector at the KEKB e+ e- collider
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Belle PID system upgrade
proximity focusing RICH with aerogel radiator in the forward direction
●n ~ 1.05●ϑC(π) = 310 mrad @ 4 GeV/c●ϑC(π) − ϑC(K) = 23 mrad @ 4 GeV/c●pion threshold 0.44 GeV/c
requirement: ~ 5σ K/πseparation @ 4 GeV/c
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Proximity focusing RICH with aerogel radiator: R+D hystory 2001-2004
Beam tests Nov. 2002 - 2004• new aerogel samples• new photon detector Hamamatsu H8500
(flat pannel PMT) with 89% eff. area• new readout electronics (1024 channels)
->NIM A518 (2004) 582
Beam Test Nov. 2001: proof of principle36 MAPMTs (R5900-M16) @ 30mm pitch, 36% eff. area, 192 readout channels
single photon Cherenkov angle resolution better than 10mrad
number of photons consistent with expectations,but clearly too low
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Beam test: Cherenkov angle resolution and number of photons
Beam test results with 4cm thick aerogel tiles in the focusing configuration: >5σ K/π separation at 4GeV/c
Hamamatsu H8500 (flat panel PMT) good for the understanding of the counter behavior intermediate step in our R+D
but: not suitable for operation in magnetic field
->e-Print: physics/0504220, to be published in NIM
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Development and testing of photon detectors for 1.5 T
Baseline: large area HPD of the proximity focusing type12x12 channels, active area 65%
-10kV15~25mm
e-
Multialkaliphotocathode
Pixel PD or APD
R&D project in collaboration with Hamamatsu
Is there a backup solution?
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Photon detector backup option: Burle MCP-PMT
BURLE 85011 MCP-PMT:
●multi-anode PMT with 2 MCPs●25 µm pores●bialkali photocathode●gain ~ 0.6 x 106
●collection efficiency ~ 60%●box dimensions ~ 71mm square●64(8x8) anode pads●pitch ~ 6.45mm, gap ~ 0.5mm●active area fraction ~ 52%
-12
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Bench test set-up
LIGHT SOURCE:●blue LED (470nm) focused by microscope to ~ 30 µm●2D position of the light source is computer controlled in steps of 12.5 µm
READOUT ELECTRONICS:●signals from anodes are amplified and discriminated by ASD8 boards●digital signals are converted to ECL levels and fed to VME modules
ASD8 = 8 channel amplifier, shaper and discriminator:●ENC ~ 900 + 70/pF●shaping time ~ 10ns●sensitivity ~ 2.5mV/fC
ASD8 BOARDS:●used in the HERA-B RICH●16 channels (2 x ASD8 chips)
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Single photon counting vs position on the tube
count rates - all channels:●charge sharing at pad boundaries
single channel response: ●uniform over pad area●extends beyond pad area (charge sharing)
2100 V
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
● variation of the counting rate at the corner of four pads
● single photon detected by 1, 2, 3 or 4 channels
5mm x 5mm, 2300 V
2100 VCharge sharing
Slice of the counting rate distribution including the central areas of 8 pads (single channels - colored, sum of all channels - black)
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Effect of photon incidence angle
Single channel response for photon incidence angles of 0o and 45o (reflections)
logarithmic scale!
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
● relative intensities of the main peak, first and second reflections are 0.92, 0.07 and 0.01 respectively
● displacement of secondary image consistent with reflection from MCP surface
● impact on spatial resolution (+10% @18o)● impact on timing resolution ∆t ~ 40ps
45o0.92
0.07
0.01
φ0
Internal reflections
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Beam test set-up
● pion beam 0.5 GeV/c - 4 GeV/c● two MWPCs for tracking● same front end electronics (ASD8) as bench tests● digital signals read out by VME TDCs● different aerogel samples used
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Beam test set-up 2
R5900-M16 characteristics:●bialkali photocathode●16 (4x4) pads, pitch 4.5mm●active area fraction ~ 36%●collection efficiency ~ 75%
● BURLE MCP-PMT mounted together with an array of 12(6x2) Hamamatsu R5900-M16 PMTs at 30mm pitch (reference counter)
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Cherenkov ring
● accumulated rings on MCP-PMT and M16 PMTs
Cherenkov photons emitted in the PMT window
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Hit clustering
Impact on -> resolution-> # of rec. photons
Charge sharing -> expect clusters instead of single hits
Number of hits per cluster
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Number of hits
# of clusters # of hits
* Poisson
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Number of hits 2
clusters●N = ~ 1.2 (@ 13%)●full ring ~ 9●full coverage ~ 4.5 (@ 52%)
photons (from Poisson zero hit probability P(0))●N = ~ 1.8 (@ 13%)●full ring ~ 14●full coverage ~ 7 (@ 52%)
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Number of hits 3
Cross-check: comparison with the reference detector
R5900-M16-PMT photons
● N = ~ 1.95 (@ 11%)● full ring ~ 17.5● full coverage ~ 6.5 (@ 36%)
MCP-PMT photons (from Poisson)
●N = ~ 1.8 (@ 13%)●full ring ~ 14●full coverage ~ 7 (@ 52%)
Photons per ring MCP-PMT: 14 R5900-M16: 17.5consistent with the ratio of collection eff. 60% vs 75%
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Resolution
● charge sharing at the edges of pads -> resolution improves if using center of gravity of the cluster
sJ: 17.8 mrad -> 13.1 mrad
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Resolution per track
● σϑ~13 mrad (single cluster)● number of clusters per track N ~ 4.5● σϑ~ 6 mrad (per track)-> ~ 4 σ π/K separation at 4 GeV/c
->marginal
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Open questions
Operation in high magnetic field:●the present tube with 25µm pores only works up to 0.8T ●for operation at 1.5T – pores size ~10µm
Number of photons per ring: too small. Possible improvements (producer):●bare tubes (52%->63%)●increase active area fraction (bare tube 63%->85%)●increase the photo-electron collection efficiency (from 60% at present up to 70%)
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Open questions
Extrapolation from the present data 4.5 hits per ring -> 8.5 σϑ per track: 6 mrad -> 4.5 mrad
-> >5 σ π/K separation at 4 GeV
-> looks OK on paper, see what Burle manages
Operation in 1.5T mag. field: test MCPs with 10µm pores
Aging of the MCP-PMTs
Can we get the 10µm tube at all???
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Summary
● BURLE MCP multianode PMT performed very well as a single photon detector both on the bench and in the test beam.
● The Cherenkov angle resolution and yield are in good agreement with expectations.
● For the specific application (RICH counter with aerogel radiator) the photon yield is too low. Improvements foreseen (larger active area fraction, collection efficiency).
R&D issues:● Testing of the versions with 10 µm pores (for operation in
B=1.5T) and with larger active area fraction. ● Photo-electron collection efficiency: 60% -> 70%?● Read-out electronics● Ageing
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Back-up slides
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Bench test set-up - electronics
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
● uniform single channel response (right)● fine scan over the boundary of 4 pads
Surface scan - details
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
MCP-PMT: Cherenkov ring & HV scan
● accumulated rings on MCP-PMT and M16 PMTs
● HV scan: number of clusters in Cherenkov ring as a function of high voltage applied to MCP-PMT
● number of clusters reaches plateau at ~ 2200V
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
MCP-PMT: hit clustering
number of clusters <number of incident photons < number of pads
NUMBER OF PADSNUMBER OF CLUSTERS An example:
● 11 pads● 7 clusters
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
MCP-PMT: number of hits 2
clusters●N = ~ 1.2 (@ 13%)●full ring ~ 9●full coverage ~ 4.5 (@ 52%)
Photons (from Poisson zero hit probability P(0))●N = ~ 1.8 (@ 13%)●full ring ~ 14●full coverage ~ 7 (@ 52%)
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Hamamatsu H8500 (flat panel PMT) as photon detector
channels)
• 8x8 multi-anode PMT (64ch) by HPK • Effective area=89% ( □49mm for □51.7mm package )• 4x4 array used in beam tests (1024 ch in total )
Not suitable for operation in magnetic field, but still good for the understanding of the detector behavior intermediate step in our R+D
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
How to increase the number of photons?
What is the optimal radiator thickness?Use beam test data on σ0 and Npe
Minimize the error per track: σ=σ0/⌦(Npe)Optimum is close to 2 cm
σ0
Npe
σ=σ0/⌦(Npe)
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Radiator with multiple refractive indices
normalHow to increase the number of photonswithout degrading the resolution?
● measure two separate rings “defocusing” configuration
● measure overlaping rings“focusing” configuration
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Beam tests
Clear rings, little background
Photon detector: array of 16 H8500 PMTs
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June 22, 2005 Beaune 2005 Photodetection Peter Križan, Ljubljana
Focusing configuration - data
4cm aerogel single index
2+2cm aerogel