Picosecond Timing Workshop - PowerPoint PPT Presentation

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Picosecond Timing Workshop

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Two inch square flat PMT with dual MCP multiplier. Anodes, 2x2, 8x8 and 32 x 32 configurations. ... 11/30/2004-12/5/2004, Playa del Carmen, Mexico ... – PowerPoint PPT presentation

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Title: Picosecond Timing Workshop


1
Discovering the Future
Sales meeting 2005
2
Production sites, US
1. PHOTONIS Key Facts
  • Lancaster, PA
  • Photomultipliers
  • Power Tubes
  • Matamoros, Mexico
  • Photomultipliers
  • Sturbridge, MA
  • Microchannel plates
  • Channel multipliers
  • Fiber optics

3
1. PHOTONIS Key Facts
Production sites, Europe
  • Brive, France
  • Photomultiplier tubes
  • Image intensifiers
  • Special products
  • Streak tubes
  • Scientific microchannel plates
  • Neutron and gamma detectors
  • Electron multipliers
  • Multichannel photomultipliers
  • Roden, Netherlands
  • Image intensifiers
  • Hybrid Photo-Diode (HPD)

4
Planacon MCP-PMTs
  • Two inch square flat PMT with dual MCP
    multiplier.
  • Anodes, 2x2, 8x8 and 32 x 32 configurations.
  • Improved Open Area Ratio device now available
  • Bi-alkali cathode on quartz faceplate.
  • Easily tiled, low profile, excellent time
    resolution, excellent uniformity.

5
PLANACON Family
  • 50mm Square family of MCP based PMTs
  • 8500X 4 anode
  • 8501X 64 anode
  • 8502X 1024 anode
  • New improved Active Area Variants available with
    86 active area, 85002/85012/85022
  • 64 anode PMT available with integrated
    Anger-logic readout
  • Gated High Voltage Power Supply available

6
Improved Open Area Ratio Planacon
  • Packaging is streamlined to maximize detector
    area relative to device dimensions
  • 2.28 sq. vs. 2.50 sq.
  • 0.45 vs. 0.65 ht.
  • 86 vs. 66 OAR
  • 68 gms vs. 128 gms

7
MCP-PMT Operation
photon
Faceplate Photocathode
Photoelectron
DV 200V
Dual MCP
DV 2000V
Gain 106
DV 200V
Anode
8
MCP-PMT Construction
Indium Seal
Faceplate
Ceramic Insulators
MCP Retainer
Dual MCP
Anode Pins
  • Spacing between faceplate and MCP and MCP and
    anode can be varied for different applications
  • Anode can be easily modified

9
PMT Processing
10
Comparison with Conventional PMT
11
Comparison with Conventional PMT
12
MCP Characteristics
  • Standard family uses 25?m pore size / 32 ?m pitch
    / 8 bias angle / 401 LD chevron
  • Prototypes have been built with 25?m pore size /
    32 ?m pitch / 8 bias angle / 601 LD chevron
  • Long-life glass
  • Standard dynamic range glass results in 50 ?A
    strip current ? Maximum average current of 5 ?A
  • Move to Extended Dynamic Range glass for 500?A
    strip current ? Maximum average current of 50 ?A
  • Collection efficiency, including first strike
    multiplication statistics, is 60 for 25µm.

13
Single Electron Spectrum
  • Good photon counting properties at gains of 0.2
    1 x 106. Currently working on increasing gain by
    2X.
  • PeakValley typically gt 21 with uniform
    illumination of faceplate.
  • Collection efficiency for single photoelectrons
    65.

14
Uniformity
  • Cathode uniformity within 10 over full active
    area.
  • Anode uniformity 1.51 over the 2 active area
    in analog mode.
  • Goal is to obtain 1.21 anode uniformity.
  • Decrease at edge of pixels due to cross-talk
  • Data provided by Jerry Vavra, SLAC

15
Spatial Variations of Detection Efficiency
C. Field, T. Hadig, David W.G.S. Leith, G.
Mazaheri, B. Ratcliff, J. Schwiening, J. Uher,
and J. Vavra
16
Timing Limitations
  • TTS limited by
  • Cathode MCP Gap and Voltage
  • Recoil electrons (cause long TT shoulder)
  • Transit time (Variations in p.e. velocity)
  • Want small gap and high field
  • MCP-Anode Gap and Voltage
  • Transit time (variations in electron velocity)
  • Marginally on recoil electrons (Broadens pulse
    width)
  • Want small gap and high field
  • Pore-size, LD, and voltage of MCP
  • Transit time variation through the pore
    (secondary emission velocity variations)
  • Want small pore size, minimum LD and high field

17
Recoil Electrons
Faceplate
pe
Recoil Electron
L
MCP
  • Scattered electrons can travel a maximum of 2L
    from initial strike
  • Produces a TTS shoulder
  • Reduces the DQE for direct detection

18
85011 430 Drop Faceplate
  • Cathode MCP gap is decreased from to 0.85mm
  • Photocathode active area is reduced to 47mm from
    50mm

19
85011 430 Drop Faceplate
20
Effect of Reduced PC-MCP Gap
21
32 Anode Timing ResolutionTiming Uniformity
  • 85011 430 (0.86mm gap) MCP-PMT shows good
  • uniformity over 32 anodes, each anode readout by
    a separate SLAC CFD channel

22
Cathode MCP Transit Time
  • Increased voltage or decreased gap can
    drastically reduce the transit time, and
    therefore transit time spread

23
Amplification in Pore
  • Typical secondary yield is 2
  • For 401 LD there are typically 10 strikes (210
    103 gain single plate)
  • Number of strikes depends on velocity of
    individual secondary electrons

24
MCP Transit Time
  • Transit time assumes 10 strike in 401 LD with
    1000V applied per plate, Chevron configuration

25
Future Directions
  • Increase the anode configurations offered
  • Improved average anode current (50 100 uA)
  • Step faceplate and anode to optimize timing
  • MCP input treatment to optimize DQE and reduce
    recoiling effect
  • Develop variants optimized for
  • Photon counting with high spatial resolution
  • Low cross-talk and magnetic field immunity
  • Cryogenic Applications
  • Ultra-low background
  • Develop other geometries as required by specific
    markets and applications
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