Identification of neutrons and gamma rays using a combination of three algorithms for separating signals of the scintillation detector

Abstract

Scintillation detectors with organic scintillators are widely used for fast neutrons detection in high gamma ray background. The peculiarity of this type of detector is that the pulse shape depends on the type of the detected particle. Traditionally, the Pulse Shape Discrimination (PSD) histogram is used to determine the number of detected neutrons. The PSD parameter is calculated from the shape of the detector pulse and assigned to each pulse. A typical PSD histogram contains two peaks corresponding to neutrons and gamma rays that overlap in the region between the peaks. With this approach, it is impossible to identify each individual signal in the area between the peaks. Therefore, it is not possible to calculate the overall signal identification coefficient. We have proposed a new method for the identification of neutrons and gamma quanta, which includes a combination of three signal separation algorithms: the traditional histogram PSD, the dependence of the area of signals on their amplitude, Tau histogram (tau means the fall constant of the detector pulses). This combination of three algorithms makes it possible to calculate the value of the signal identification coefficient. To test a new method for identifying neutrons and gamma quanta, we used a Pu-Be neutron source, a scintillation detector with a p-terphenyl crystal and a CAEN DT5730 Digitizer (14 bit, 500 MHz). When a scintillation detector registered neutron from a Pu-Be source, the signal identification coefficient was 91.6%. A new method for identifying signals from a scintillation detector is used to register neutrons at the light ion accelerator.

Investigation of Neutron Generation upon Irradiation of Deuterated Crystalline Structures with an Electron Beam

“…Scintillation detectors based on a p-terphenyl crystal (diameter 2.5 cm, height 2.5 cm) were equipped with a Hamamatsu R6094 photomultiplier. The technique of separating signals from neutrons and gamma quanta by the shape of the scintillation detector pulses is described in [13,14]. Deuterated targets made of palladium and textured CVD diamond were used in the experiment.…”