<p>Three configurations shown for a 2×2×20 mm<sup>3</sup> LSO:CeCa scintillator crystal. In this we see that the partially wrapped and wrapped configurations shown good alignment, whereas the unwrapped shows poor. This will result in fewer events being collected and thus a larger error in higher DOI measurements.</p
<p>The two timing coincidence apparatuses. In (a) the standard coincidence apparatus, used in this p...
The properties of a 50 mm x 50 mm x 30 mm monolithic LaBr3:Ce scintillator crystal coupled to a posi...
The uncertainty in time of particle detection within a scintillator detector, characterised by the c...
<p>The coincidence time resolution is plotted versus the depth of interaction for three configuratio...
<p>The energy resolution (%) for a LSO:CeCa scintillator crystal of shape 2×2×20 mm<sup>3</sup> for ...
<p>The right photopeak centroid plotted against the depth of interaction for a LSO:CeCa scintillator...
<p>The delay peak position with depth of interaction is plotted for a LSO:CeCa scintillator crystal ...
<p>The right photopeak centroid versus the depth of interaction for two identical LYSO:Ce scintillat...
<p>The number of <i>γγ</i> events recorded with DOI for two Proteus 2×2×30 mm<sup>3</sup> LYSO:Ce sc...
A Monte Carlo simulation of a 50mm×50mm×4mm continuous crystal has been developed to investigate the...
The scintillation crystal block for a positron emission tomography (PET) detector is generally compo...
<p>All measurements conducted with 2x2x20mm3, 2x2x30mm3 Proteus LYSO:Ce and 2x2x20mm3 Agile LSO:CeCa...
<p>The timing coincidence apparatus set up for DOI measurements. The reference detector, shown on th...
<p>The delay peak centroid versus the depth of interaction plotted for two Proteus 2×2×30 mm. LYSO:C...
none15Knowledge of the Depth-Of-Interaction (DOI) in detector is crucial for small ring diameter PET...
<p>The two timing coincidence apparatuses. In (a) the standard coincidence apparatus, used in this p...
The properties of a 50 mm x 50 mm x 30 mm monolithic LaBr3:Ce scintillator crystal coupled to a posi...
The uncertainty in time of particle detection within a scintillator detector, characterised by the c...
<p>The coincidence time resolution is plotted versus the depth of interaction for three configuratio...
<p>The energy resolution (%) for a LSO:CeCa scintillator crystal of shape 2×2×20 mm<sup>3</sup> for ...
<p>The right photopeak centroid plotted against the depth of interaction for a LSO:CeCa scintillator...
<p>The delay peak position with depth of interaction is plotted for a LSO:CeCa scintillator crystal ...
<p>The right photopeak centroid versus the depth of interaction for two identical LYSO:Ce scintillat...
<p>The number of <i>γγ</i> events recorded with DOI for two Proteus 2×2×30 mm<sup>3</sup> LYSO:Ce sc...
A Monte Carlo simulation of a 50mm×50mm×4mm continuous crystal has been developed to investigate the...
The scintillation crystal block for a positron emission tomography (PET) detector is generally compo...
<p>All measurements conducted with 2x2x20mm3, 2x2x30mm3 Proteus LYSO:Ce and 2x2x20mm3 Agile LSO:CeCa...
<p>The timing coincidence apparatus set up for DOI measurements. The reference detector, shown on th...
<p>The delay peak centroid versus the depth of interaction plotted for two Proteus 2×2×30 mm. LYSO:C...
none15Knowledge of the Depth-Of-Interaction (DOI) in detector is crucial for small ring diameter PET...
<p>The two timing coincidence apparatuses. In (a) the standard coincidence apparatus, used in this p...
The properties of a 50 mm x 50 mm x 30 mm monolithic LaBr3:Ce scintillator crystal coupled to a posi...
The uncertainty in time of particle detection within a scintillator detector, characterised by the c...