High resolution imaging with MCP detectors using delay line anodes

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Transcript High resolution imaging with MCP detectors using delay line anodes

High resolution imaging with MCP detectors using delay line anodes

Ottmar Jagutzki, Uwe Spillmann, Achim Czasch Horst Schmidt Böcking, Reinhard Dörner, … In collaboration with Volker Dangendorf from PTB Braunschweig, Neutron Radiography group

The helical wire delay-line anode

DLD40

Sobottka and Williams 1988

Fast timing electronics high rate, multi-hit

5(7) electronic channels only easy read-out

Center-of-mass averaging

high position resolution time resolution: < 1 ns Our typical resolution: 40-50 μm rms

80 mm “Hexanode” delay-line detector (patented)

Electronic readout:

T

ime-to-

D

igital-

C

onverter:

(old) Wilkinson-type analog-digital conversion (like a TAC): high resolution but a slow digital conversion  “counter”-type fast (no!) conversion: Pretty high resolution and fast read-out resolution limited by clock rate

TDC8HP:

PC-controlled multi-hit TDC with 8 channels, 25 psec LSB, stable read-out speed : 400 kHz now, up to 2 MHz planned ( < 10 ns dead-time between hits ) “TDCHP” chip developed by CERN

How to detect visible/near-UV photons with that ?

Photek 75 mm image intensifier with RoentDek DL80 anode 5 mm grid constant, 1 mm obstacle NASA test mask 0.15 mm FWHM 0.075 mm pixel (rms) Now: < 40 micron rms

Counting/Imaging near-UV and visible photons with delay-line read-out

DL40-PMT

Quartz window Photo cathode MCP stack DL40 anode (or bigger) works fine, but - difficult to build - not very robust (?) - size up to 150 mm possible?

Counting/Imaging near-UV and visible photons with delay-line read-out via image charge pick-up : the

RS-PMT

Quartz window Photo cathode MCP stack Resistive screen pickup electrode (e.g. delay-line) - easy, robust design of detector head - size up to 40 mm, may be bigger - standard (multi-layer) PCB pickup electrodes Patented technique Image charge read-out: Battistoni et al. 1982

Counting/Imaging near-UV and visible photons with reconfigurable read-out Read-out technique can easily be reconfigured using the same detector head. Patented technique Quartz window Photo cathode MCP stack Resistive screen other pickup electrodes: Wedge&Strip, Pixel,…

Counting/Imaging VUV photons or particles with reconfigurable read-out

“open RS-PMT”

Image charge read-out has some advantages over charge collection for some anodes: Beneficial even for open-face detectors Patented technique MCP stack Resistive screen pickup electrodes: Delay-line, Wedge&Strip, Pixel, …

Delay-line read-out of RS-PMT: Multilayer PCB Front and rear side “antennas” (Eland 1994) connected to delay-line: (Berkeley group) LC-delay-line

LC-DL50 on open RS-PMT40, irradiated with α – particles, mesh obstacle 80 micron

LC-DL50 on open RS-PMT40, irradiated by ions with 500 kHz , mesh obstacle 80 micron

LC-DL50 on open RS-PMT40, irradiated by ions with 500 kHz , mesh obstacle 80 micron

8 x 8 mm linear scale log scale

Hexanode for RS-PMT

: - multi-hit (simultaneous photon pair detection is possible): Compton telescope?

intrinsic linearity correction (no test mask necessary): 3 combination for determining x- and y-coordinates from u, v, w coordinate system Example for x-layer: x = u = - (v + w) (over-determination) (vector addition) v w u x = u But how can this help correcting non-linearity ?

50 mm LC Hex-DL on a 4-layer PCB

Linearity correction

of LC-delay-line: (no mask needed) of RS-PMT: 60 40 20 0 140 120 100 80 16 2,0 mm 18 20 position / mm Experiment 4 (d=1.0 mm) Gauss Fit X c =18.9 mm s =0.86 mm 22

Summary:

- Large (open-face) MCP delay-line detector with up to 3000x3000 pixel - Resistive screen PMT or open MCP detector for counting photons (might qualify for space) - redundant triple-layer delay-line anode read-out with intrinsic linearity correction - read-out anodes can easily by swapped work to be done: - position resolution needs to be improved for the 40 mm and 25 mm formats - no experience with flight mission - not much experience with photon counting at all !

Applications: - FLIM (fluorescence life-time microscopy) - NEURRAD (element sensitive neutron radiography) in cooperation with Volker Dangendorf, PTB Braunschweig Thanks to Jürgen Barnstedt from Tübingen for borrowing us his RS-PMT!

Results of Barnstedt et al. (1998) 25mm RS-PMT (Proxitronic) - bi-alkali photo-cathode - 4-jaw Wedge&Strip anode Projection of grid mask 70/600micron, resolution 35 micron (1:700)