Method for determining the neutron flux by using a portable radionuclide identification device (RID) comprising scintillation material with iodine

1. A method for determining neutron flux by utilizing a portable Radionuclide Identification Device (RID) wherein the RID comprises an inorganic crystal, a light detector and electronics adapted to evaluate the output signals of the light detector, the method comprising:

detecting light emitted by the crystal based on events that comprise radiation induced interactions with the crystal using the light detector, wherein the light detector measures an intensity of the light as a function of energy deposed in the crystal by said events;

determining the energy deposed in the crystal by evaluating a pulse height of the output signal of the light detector;

selecting a first group of said events in a first energy window, wherein the first energy window comprises events having energies that exceed a minimum first threshold energy, E T1 ;

selecting a second group of said events in a second energy window, W(n,μ),

wherein the second energy window comprises events having energies above a second threshold energy, E T2 , and below a third threshold energy, E T3 , and wherein E T3 is less than or equal to E T1 ;

determining a count rate R(μ) of the first group of said events,

determining a count rate R(n,μ) of the second group of said events,

determining, for each measurement for determining neutron flux, a background count rate R(back) from an expected count rate R(μ) exp of interactions of the cosmic radiation with the crystal in the second energy window W n,μ), wherein said expected count rate R(μ) exp is being calculated from the count rate R(μ) and a known energy distribution of cosmic radiation; and

determining a neutron flux count rate R(n) by subtracting the background count rate R(back) from the count rate R(n,μ).

2. The method of claim 1 , wherein the crystal is selected from a group of sodium iodide and cesium iodide.

3. The method of claim 1 , wherein the first threshold energy is 10 MeV.

4. The method of claim 1 , wherein the second threshold energy is 3 MeV.

5. The method of claim 1 , wherein the third threshold energy is 5 MeV.

6. The method of claim 1 , wherein the count rate R(back) is further corrected by adding a count rate of pileup events R(n,μ) pileup within the second energy window W(n,μ).

7. The method of claim 6 , wherein the count rate of pileup events R(n,μ) pileup is calculated by multiplying a calculated pileup count rate R(n,μ) sum in the second energy window W(n,μ) with a mean count rate r and a pulse pair resolving time t ppr .

8. The method of claim 7 , wherein the expected count rate of pileup events R(n,μ) sum is calculated from a count rate of events built by the sum of two consecutive random events in the second energy window W(n,μ).

9. The method of claim 1 , wherein an alarm is generated when the neutron flux count rate R(n) increases above a threshold rate within a predetermined time, said threshold rate being calculated from the actual background count rate R(back).

10. A portable radionuclide identification device (RID), comprising an inorganic crystal, a light detector, and electronics adapted to evaluate the output signals of the light detector, characterized in that the electronics are adapted to evaluate signals being equivalent to energies deposited in the crystal of more than 5 MeV and that the RID is adapted to conduct a method for determining the neutron flux according to claim 1 .

11. The method of claim 1 , wherein E T1 is defined such that, in the first energy window, a majority of the events originate from interactions with cosmic radiation.

12. The method of claim 1 , wherein E T2 is higher than a maximum energy deposed by gamma radiation E(γ) max to be measured.