Radiation detection system and method of analyzing an electrical pulse output by a radiation detector

1. A radiation detection system comprising:

a photosensor to receive light from a scintillator via an input and to send an electrical pulse at an output in response to receiving the light; and

a pulse analyzer comprising a circuit that is adapted to calculate the integral over time of at least a portion of a decay portion of an electrical pulse and the integral over time of the combination of the decay portion and a rise portion of the electrical pulse and to determine whether the electrical pulse corresponds to a neutron-induced pulse, based on a ratio of the integral of at least a portion of the decay portion of the electrical pulse to an integral of a combination of the decay portion and the rise portion of the electrical pulse.

2. The radiation detection system of claim 1 , wherein the pulse analyzer is configured to compare the ratio with a predetermined value and to identify the electrical pulse as a neutron-induced pulse when the ratio is at least the predetermined value.

3. The radiation detection system of claim 2 , wherein the pulse analyzer is configured to return the ratio as a variable and to compare the variable to the predetermined value.

4. The radiation detection system of claim 1 , wherein the decay portion and the rise portion include portions of the electrical pulse that are at or above a threshold.

5. The radiation detection system of claim 1 , wherein the combination of the decay portion and the rise portion includes a peak of the electrical pulse.

6. The radiation detection system of claim 1 , wherein the combination of the decay portion and the rise portion includes a peak integration window defined by a first time that corresponds to a highest reading of the electrical pulse and a second time that corresponds to a reading that is immediately before or immediately after the highest reading.

7. The radiation detection system of claim 6 , wherein a peak integration window has a width that is adjustable at the pulse analyzer.

8. The radiation detection system of claim 1 , wherein the pulse analyzer includes a field programmable gate array (FPGA).

9. The radiation detection system of claim 1 , wherein the pulse analyzer is configured to send an indicator to a pulse processing device, wherein the indicator indicates whether the electrical pulse corresponds to the neutron-induced pulse or to the gamma radiation-induced pulse.

10. The radiation detection system of claim 9 , wherein the indicator comprises a first replicate of the electrical pulse.

11. The radiation detection system of claim 10 , wherein the first replicate comprises an analog replicate of the electrical pulse.

12. The radiation detection system of claim 10 , wherein the pulse analyzer includes:

a splitter to replicate the electrical pulse and to send the first replicate to a delay circuit and to send a second replicate to a pulse analysis device; and

an output control circuit to receive the first replicate from the delay circuit after the pulse analysis device has calculated the integrals, wherein the output control circuit is configured to send the first replicate to the first output after receiving a logic pulse from the pulse analysis device and to send the first replicate to the second output when a logic pulse is not received from the pulse analysis device.

13. The radiation detection system of claim 1 wherein the digital logic circuit comprises a field programmable gate array.

14. A method comprising:

receiving an electrical pulse at a pulse analyzer from a photosensor of a radiation detection device;

defining a peak integration window to include a highest reading of the electrical pulse and another reading immediately before or immediately after the highest reading;

determining whether the electrical pulse corresponds to a neutron-induced pulse or a gamma radiation-induced pulse, based on a ratio of an integral of a particular portion of the electrical pulse to an integral of a combination of a decay portion and a rise portion of the electrical pulse, wherein each of the integrals is integrated over time and the decay portion and the rise portion are at or above a threshold; and

sending an indicator to a pulse processing device, the indicator identifying the electrical pulse as corresponding to a neutron-induced pulse or a gamma radiation-induced pulse.

15. The method of claim 14 , wherein the particular portion consists of the decay portion.

16. The method of claim 14 , further comprising comparing the ratio with a predetermined value and identifying the electrical pulse as a neutron-induced pulse when the ratio is at least the predetermined value.

17. The method of claim 14 , wherein the peak integration window has a width that is at most 2 ns.

18. A method comprising:

receiving a first electrical pulse from a photosensor of a radiation detection device;

replicating the first electrical pulse to form a second pulse;

sending the first electrical pulse to a pulse analysis device and sending the second pulse to a delay circuit;

calculating with the pulse analysis device a ratio of the integral over time of the particular portion of the first electrical pulse to the integral over time of the total pulse and comparing the ratio to a predetermined value, in order to determine whether the electrical pulse corresponds to a neutron-induced electrical pulse or a gamma radiation-induced electrical pulse; and

sending a logic pulse from the pulse analysis device to an output control circuit indicating that the electrical pulse corresponds to a neutron-induced electrical pulse when the ratio is at least a predetermined value.

19. The method of claim 18 , further comprising:

receiving the second pulse at the output control circuit after the pulse analysis device has calculated the integrals; and

sending the second electrical pulse to a first output after receiving a logic pulse from the pulse analysis device indicating that the electrical pulse corresponds to a neutron-induced electrical pulse and sending the second pulse to a second output when the logic pulse from the pulse analysis device is not received.

20. The method of claim 18 , further comprising:

receiving the second pulse at the output control circuit after the pulse analysis device has calculated the integrals; and

sending the second electrical pulse to a first output after receiving a logic pulse from the pulse analysis device indicating that the electrical pulse corresponds to a neutron-induced electrical pulse and sending the second pulse to a second output after receiving a logic pulse from the pulse analysis device indicating that the electrical pulse corresponds to a gamma radiation-induced electrical pulse.