<?xml version="1.0"?>
<metadata xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/"><dc:title>Cerenkov PET detector based on silicon photomultipliers</dc:title><dc:creator>Consuegra Rodríguez,	Dania	(Avtor)
	</dc:creator><dc:creator>Korpar,	Samo	(Mentor)
	</dc:creator><dc:subject>PET</dc:subject><dc:subject>Cherenkov</dc:subject><dc:subject>PbF2</dc:subject><dc:subject>TOF</dc:subject><dc:subject>CTR</dc:subject><dc:subject>SiPM.</dc:subject><dc:description>The use of Cherenkov light in positron emission tomography (PET) has the potential
to improve the time-of-fight (TOF) resolution and reduce the cost of detectors.
Lead fuoride (PbF2) has emerged as a highly performing radiator material suitable
for TOF-PET application due to its excellent gamma stopping power and optical
properties. Previous studies using coincidences between a small number of crystals
have shown good performance in terms of coincidence time resolution (CTR). In
this work, the feasibility of Cherenkov TOF-PET is studied in detail, extending the
number of channels and optimizing the detectors for better performance. Simulations
were used to study different detector geometries and PbF2 crystal optical surface
treatments, up to a whole-body PbF2 TOF-PET scanner. The simulation data
showed that the quality of reconstructed images obtained when using different
Cherenkov TOF-PET scanner geometries is comparable to current state-of-theart
scintillator scanners. Experiments with different detector confgurations were
carried out to measure CTR and e ciency. The HRFlexTOT electronics enabled
measurements of coincidences between two Cherenkov TOF-PET modules placed
in a back-to-back confguration with up to 16 channels per module. Of particular
interest is a multi-layer detector geometry, which improves the TOF resolution and
reduces the parallax error without compromising the detection e ciency. With a
multi-layer detector geometry, the CTR of the simulated whole-body PbF2 TOFPET
scanner was 143 ps, out of which the fundamental limitation due to light
production and transportation was only 22 ps. Experimentally, such CTR value
could not yet be achieved due to the limited performance of silicon photomultiplier
photodetectors currently available. With further development of the photodetectors
and the readout electronics, Cherenkov TOF-PET could become a competitive
reality in PET.</dc:description><dc:date>2022</dc:date><dc:date>2022-10-21 08:15:01</dc:date><dc:type>Doktorsko delo/naloga</dc:type><dc:identifier>142139</dc:identifier><dc:identifier>VisID: 128773</dc:identifier><dc:identifier>COBISS_ID: 128062723</dc:identifier><dc:language>sl</dc:language></metadata>
