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@INPROCEEDINGS{Streun:201246,
author = {Streun, M. and Nöldgen, Holger and Erven, A. and Espana,
S. and Jokhovets, L. and Marcinkowski, R. and Peters, C. and
Ramm, M. and Schramm, N. and Wüstner, Peter and
Vandenberghe, S. and Kemmerling, G. and van Waasen, S.},
title = {{PET} {S}cintillator {A}rrangement on digital {S}i{PM}s},
reportid = {FZJ-2015-03551},
isbn = {978-1-4799-0534-8},
pages = {4},
year = {2014},
abstract = {The common way to build a PET detector is to place an array
of scintillator elements on top of a photo detector. In
order to achieve high spatial resolution the scintillator
footprints are often smaller than the pixel size of the
photodetector. This requires light sharing and some kind of
algorithm like Anger-Logic in order to identify the correct
scintillator element in which the event took place. The
digital Silicon Photomultiplier DPC3200-22-44 (Philips
Digital Photon Counting) is a fully digital photo sensor
device [1]. Each pixel consists of 3200 individual micro
cells which are charged and read out under digital control.
The device (Tile) is organized as an array of 8 by 8 pixels
each of 3.9x3.9 mm2 size and is realized as a PCB equipped
with 16 dice. One die provides four pixels together with the
corresponding triggering, validation and readout
electronics. Depending on the configuration the detection of
an event on one die can cause the other dice to transmit
their data as well (neighbor logic). The obvious solution of
using neighbor logic and a scintillator matrix with light
guide covering the whole tile shows some drawbacks. After
each event all 16 dice will be busy and all pixels need to
be read out. This results in increased dead time and a lot
of data. Furthermore it turned out that sometimes pixels are
missing because dice were already busy and could not
transmit data when the event was detected. This will
complicate the identification of the event position. A
better performance can be obtained when the light is shared
only within the four pixels of each die and the dice work
independent from each other. We investigated the positioning
capability of different scintillator matrices and light
guides. These are arranged in such a way, that a single die
can only receive the light from a 4 by 4 array of LYSO
crystals which covers exactly the die dimensions. The
results show that clear crystal identification can be
achieved with such an arrangement. [1] Haemisch et al.,
Physics Procedia 37 (2012) 1546},
month = {Oct},
date = {2015-10-27},
organization = {2013 IEEE NUCLEAR SCIENCE SYMPOSIUM
AND MEDICAL IMAGING CONFERENCE, Seoul
(Korea), 27 Oct 2015 - 2 Nov 2015},
cin = {ZEA-2},
cid = {I:(DE-Juel1)ZEA-2-20090406},
pnm = {89582 - Plant Science (POF2-89582)},
pid = {G:(DE-HGF)POF2-89582},
typ = {PUB:(DE-HGF)8},
url = {https://juser.fz-juelich.de/record/201246},
}