Photon correlations in positron annihilation

Gauthier, Isabelle; Hawton, Margaret

doi:10.1103/physreva.81.062121

Cited by 3 publications

(1 citation statement)

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“…The desired ToF information is t flight degraded by t DoI , t OTT and t CTT , and their associated variances, as shown in figure 2. Additional factors affecting the time information, such as quantum mechanical limits in the emission of the two annihilation photons (Irby 2003, Gauthier andHawton 2010) are part of a separate investigation. The ToF difference of the two annihilation photons t which is used to extract position information x for event localization along a ToR is directly proportional to x when the scintillation photons are produced at the same depth in both crystals and do not encounter scatter at the crystal interfaces prior to detection (figure 2, top):…”

Section: Physical Parameter Modelingmentioning

confidence: 99%

Investigating the temporal resolution limits of scintillation detection from pixellated elements: comparison between experiment and simulation

Spanoudaki

Levin

2011

Phys. Med. Biol.

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This study investigates the physical limitations involved in the extraction of accurate timing information from pixellated scintillation detectors for positron emission tomography (PET). Accurate physical modeling of the scintillation detection process, from scintillation light generation through detection, is devised and performed for varying detector attributes, such as the crystal element length, light yield, decay time and surface treatment. The dependence of light output and time resolution on these attributes, as well as on the photon interaction depth (DoI) of the annihilation quanta within the crystal volume, is studied and compared with experimental results. A theoretical background which highlights the importance of different time blurring factors for instantaneous ('ideal') and exponential ('realistic') scintillation decay is developed and compared with simulated data. For the case of a realistic scintillator, our experimental and simulation findings suggest that dependence of detector performance on DoI is more evident for crystal elements with rough ('as cut') compared to polished surfaces (maximum observed difference of 64% (25%) and 22% (19%) in simulation (measurement) for light output and time resolution, respectively). Furthermore we observe distinct trends of the detector performance dependence on detector element length and surface treatment. For short crystals (3 × 3 × 5 mm(3)) an improvement in light output and time resolution for 'as cut' compared to polished crystals is observed (3% (7%) and 9% (9%) for simulation (measurement), respectively). The trend is reversed for longer crystals (3 × 3 × 20 mm(3)) and an improvement in light output and time uncertainty for polished compared to 'as cut' crystals is observed (36% (6%) and 40% (20%) for simulation (measurement), respectively). The results of this study are used to guide the design of PET detectors with combined time of flight (ToF) and DoI features.

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Section: Physical Parameter Modelingmentioning

confidence: 99%