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The UC Simulation of Picosecond Detectors

The UC Simulation of Picosecond Detectors. Pico-Sec Timing Hardware Workshop November 18, 2005 Timothy Credo. TOF Detection. Current method: bars of scintillator several meters long Signal amplified in PMT at each end Relevant length scale is 1 in, which governs time resolution (100 ps)

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The UC Simulation of Picosecond Detectors

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  1. The UC Simulation of Picosecond Detectors Pico-Sec Timing Hardware Workshop November 18, 2005 Timothy Credo

  2. TOF Detection • Current method: bars of scintillator several meters long • Signal amplified in PMT at each end • Relevant length scale is 1 in, which governs time resolution (100 ps) • 1 picosecond resolution requires scale on the order of 300 microns

  3. A Picosecond TOF Detector • Light produced in the window of MCP-PMT shines on a photocathode • Signal amplified in MCP, and summed in the anode • Electronics measure pulse from four collection points

  4. Summing Multianode • Multilayer circuit board collects MCP signal • 16x16 125 micron pads each routed to electronics by equal-time impedance-matched traces • 4 central collection points deliver signal to electronics • Mismatched impedances cause signal reflections

  5. Simulations (Window, MCP) • Cherenkov emission, transmission, chromatic dispersion, and quantum efficiency simulated in ROOT (started by R. Schroll) • Simulations use MCP time spread and gain (1e6) for single photons to estimate the signal arriving on the anode • These data were input into an HSPICE simulation of the summing anode

  6. Window Thickness and Material • Simulations evaluated the time resolution of the window and MCP for different window materials and thicknesses • MgF2 is transparent further into the ultraviolet and offers better performance • Larger windows generate more photons, providing a better average over TTS

  7. Time Resolution (Window, MCP) • The time resolution of the window and MCP depend on the number of photons detected and on the TTS of the MCP • With the Burle Planacon MCP, simulations indicate a 6 picosecond resolution • A smaller TTS (already achieved in smaller area MCPs) would make 1 ps resolution possible Average timing of signals arriving at the anode, for different MCPs

  8. Simulations (Anode) • The performance of the multianode was simulated in HSPICE using a spice model generated from the board design using HyperLynx • With a 50 Ωtermination, ringing decayed with a time constant of τ = 5.5 ns • With 60 ps TTS, pulse had average rise time of 80 ps, and average height .25 V • With 10 ps TTS, average rise time was 25 ps, and average height 1.2 V Voltage vs. time plots of anode simulations, with 60 ps TTS (top) and 10 ps TTS (bottom)

  9. Ten Simulated Pulses (60 picosecond TTS)

  10. Ten Simulated Pulses (10 picosecond TTS)

  11. Time Resolution (Anode) • With a large TTS (σ = 60 ps), the pulse shape is not consistent • With this anode a resolution of around 10 to 20 picoseconds could be achieved for a large TTS • With a faster MCP, the pulse shape is more stable • Picosecond resolution may be possible, but not without a fast large area MCP (TTS comparable to smaller area MCPs)

  12. Future Plans • Custom summing board mates with standard 32x32 Burle anode • Glue boards to Burle PMT with Planacon MCP using conductive epoxy (Greg Sellberg, Fermilab) • Solder component board with fast comparators • Use commercial TDC(?) and test several tubes in a beam at Fermilab or Argonne

  13. Conclusion and Questions • A picosecond TOF detector could be developed, but would rely on a fast large area MCP and fast electronics • Is the MCP response to a single photoelectron a good approx. to its behavior in the case of many photoelectrons? • Will the particle create a pulse as it passes through the anode and the electronics, and what effect will this have?

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