Gamma ray spectroscopy employing divalent europium-doped alkaline earth halides and digital readout for accurate histogramming
According to one embodiment, a scintillator radiation detector system includes a scintillator, and a processing device for processing pulse traces corresponding to light pulses from the scintillator, where the processing device is configured to: process each pulse trace over at least two temporal windows and to use pulse digitization to improve energy resolution of the system. According to another embodiment, a scintillator radiation detector system includes a processing device configured to: fit digitized scintillation waveforms to an algorithm, perform a direct integration of fit parameters, process multiple integration windows for each digitized scintillation waveform to determine a correction factor, and apply the correction factor to each digitized scintillation waveform.
1. A scintillator radiation detector system, comprising:
a scintillator; and
a processing device for processing pulse traces corresponding to light pulses from the scintillator, wherein the processing device is configured to: process each pulse trace over at least two temporal windows and to use pulse digitization to improve energy resolution of the system.
2. The scintillator radiation detector system of claim 1 , wherein the processing device is further configured to: determine a correction factor based on processing the at least two temporal windows and apply the correction factor to each pulse trace.
3. The scintillator radiation detector system of claim 1 , wherein the processing device is configured to fit each pulse trace using an algorithm to process the pulse traces, wherein the algorithm includes fitting each of the pulse traces to at least an exponential decay.
4. The scintillator radiation detector system of claim 3 , wherein the processing device is further configured to perform an analytic integration of parameters describing the exponential decay.
5. The scintillator radiation detector system of claim 3 , wherein the algorithm further includes fitting each of the pulse traces to an exponential rise and the exponential decay.
6. The scintillator radiation detector system of claim 5 , wherein the processing device is further configured to perform an analytic integration of parameters describing the exponential rise and the exponential decay.
7. The scintillator radiation detector system of claim 1 , wherein the pulse digitization improves the energy resolution of the system at 662 keV by at least 0.3%.
8. The scintillator radiation detector system of claim 1 , wherein the energy resolution of the system at 662 keV is less than 4%.
9. The scintillator radiation detector system of claim 1 , wherein the scintillator is a europium-doped alkaline earth halide.
10. The scintillator radiation detector system of claim 1 , wherein the scintillator has a volume greater than 1 cm 3 .
11. The scintillator radiation detector system of claim 1 , wherein the scintillator has a volume greater than 10 cm 3 .
12. The scintillator radiation detector system of claim 1 , wherein the processing device includes a Field Programmable Gate Array (FPGA).
13. A scintillator radiation detector system, comprising:
a processing device configured to:
fit digitized scintillation waveforms to an algorithm;
perform a direct integration of fit parameters;
process multiple integration windows for each digitized scintillation waveform to determine a correction factor; and
apply the correction factor to each digitized scintillation waveform.
14. The scintillator radiation detector system of claim 13 , wherein an energy resolution of the system at 662 keV is less than 4%.
15. The scintillator radiation detector system of claim 13 , wherein the algorithm includes processing at least an exponential decay for each of digitized waveform.
16. The scintillator radiation detector system of claim 13 , wherein the algorithm is an Aτ algorithm represented by:
A [exp(−t/τ D ) −exp(−t/τ R )]
where A is an amplitude of a digitized scintillation waveform, t is a sampling period, τ D is a decay time, and τ R is a rise time.
17. The scintillator radiation detector system of claim 13 , wherein the digitized scintillation waveforms are derived from light pulses from a scintillator.