Geant4 Analysis of a Thermal Neutron Real-Time Imaging System

• Published in: IEEE transactions on nuclear science 2017-07, Vol.64 (7), p.1652-1658
• Main Authors: Datta, Arka, Hawari, Ayman I.
• Format: Article
• Language: English
• Subjects: Absorption; Alpha rays; Charge coupled devices; Charged particles; Collimation; Computer simulation; Engineering; Experimental nuclear reactors; Geant4; Imaging; Neutron absorption; Neutron beams; neutron imaging; Neutrons; Nondestructive testing; Optical filters; Optical imaging; Particle physics; Photonics; Photons; Radiographs; Radiography; Reaction products; Real time; Recording; Sapphire; scintillator; Scintillators; Screens; Simulation; Spatial resolution; Thermal imaging; Triton; Zinc sulfide
• ISSN: 0018-9499; 1558-1578
• DOI: 10.1109/TNS.2017.2708031

Thermal neutron imaging is a technique for nondestructive testing providing complementary information to X-ray imaging for a wide range of applications in science and engineering. Advancement of electronic imaging systems makes it possible to obtain neutron radiographs in real time. This method requires a scintillator to convert neutrons to optical photons and a charge-coupled device (CCD) camera to detect those photons. Alongside, a well collimated beam which reduces geometrical blurriness, the use of a thin scintillator can improve the spatial resolution significantly. A representative scintillator that has been applied widely for thermal neutron imaging is 6 LiF:ZnS (Ag). In this paper, a multiphysics simulation approach for designing thermal neutron imaging system is investigated. The Geant4 code is used to investigate the performance of a thermal neutron imaging system starting with a neutron source and including the production of charged particles and optical photons in the scintillator and their transport for image formation in the detector. The simulation geometry includes the neutron beam collimator and sapphire filter. The 6 LiF:ZnS (Ag) scintillator is modeled along with a pixelated detector for image recording. The spatial resolution of the system was obtained as the thickness of the scintillator screen was varied between 50 and 400 μm. The results of the simulation were compared to experimental results, including measurements performed using the PULSTAR nuclear reactor imaging beam, showing good agreement. Using the established model, further examination showed that the resolution contribution of the scintillator screen is correlated with its thickness and the range of the neutron absorption reaction products (i.e., the alpha and triton particles). Consequently, thinner screens exhibit improved spatial resolution. However, this will compromise detection efficiency due to the reduced probability of neutron absorption.