Author:
Mehadji Brahim,Dupont Mathieu,Montrot Adrien,Roncali Emilie,Morel Christian,Farman Bardia
Abstract
Abstract
The fields of radio-guided surgery and interventional
nuclear medicine benefit from a growing array of technologies that
aid novel healthcare interventions. Among them, surgery probes able
to efficiently detect β
+ emitters are essential to localize
tumors previously detected in PET images. Different methods have
been proposed for 18F radio-guidance within the body such as
detection of 511 keV annihilation photons using electronically or
mechanically collimated probes. The main limitations to the
widespread use of these techniques are the lack of precise
directional capabilities and inadequate sensitivity. We first used
the Monte Carlo simulation platform GATE to determine the optimal
signal to noise ratio that can be achieved with an ideal probe.
Then, we focused on investigating a small Compton-angles collimation
prototype probe followed by the construction of an initial proof of
concept demonstrator. The performance of the small Compton-angles
collimation probe was compared with a commercial probe based on
mechanical collimation in terms of sensitivity and
directionality. Monte Carlo simulations showed that in case of an
ideal probe, with a tumor of 1 cm diameter positioned 5 mm under
the skin and with a SUV of 2, the measured signal to background
ratio would be of the order of 25%. The small Compton-angles
collimated probe prototype showed significantly improved
directionality compared to the commercial probe with mechanical
collimation, despite having a sensitivity lower than the commercial
probe. Monte Carlo simulations provide insights into the substantial
impact of the background on the measured signal. Furthermore, the
application of small Compton-angles collimation yields promising
outcomes, particularly in terms of improving the directionality,
with the objective of enhancing the detection of tumors. In
addition, the studied prototype probe sensitivity can possibly be
improved by upgrading the detector crystal material and geometry.