Method of luminescent solid state dosimetry of mixed radiations
A method of determining the doses of neutrons, gamma and X-ray photons, beta, alpha and other ionizing radiations using a method of image processing in spatial and frequency domain that produces parameters that are related to the radiation dose absorbed in a luminescent material. Portions of the luminescent material may be covered by different converters to allow for doses of different radiations to be discriminated.
1. A method comprising the following steps:
(a) providing a depth profile of track density for one or more radiations based on measurements of one or more high spatial resolution fluorescence images at different depths below a surface of a luminescent material covered by one or more converters; and
(b) determining a median energy of one or more radiations based on the depth profile of track density;
wherein the fluorescence images are generated by the one or more converters being exposed to the one or more radiations.
2. The method of claim 1 , wherein step (b) comprises determining the depth at which the track density is reduced to a selected level that is a selected fraction of the level of the track density at the surface of the luminescent material.
3. The method of claim 1 , wherein the method comprises the following step:
(c) obtaining the measurements by measuring the high spatial resolution fluorescence images at different depths below the surface of the luminescent material.
4. A method comprising the following steps:
(a) providing a depth profile of a power spectrum integral for one or more radiations based on measurements of one or more high spatial resolution fluorescence images at different depths below a surface of a luminescent material covered by one or more converters; and
(b) determining a median energy of one or more radiations based on the depth profile of the power spectrum integral;
wherein the fluorescence images are generated by the one or more converters being exposed to the one or more radiations.
5. The method of claim 4 , wherein step (b) comprises determining the depth at which the power spectrum integral is reduced to a selected level that is a selected fraction of the level of the power spectrum integral at the surface of the luminescent material.
6. The method of claim 4 , wherein the method comprises the following step:
(c) obtaining the measurements by measuring the high spatial resolution fluorescence images at different depths below the surface of the luminescent material.
7. A method comprising the following steps:
(a) providing a first value of track density and a second value of track density for a radiation field; and
(b) determining a median energy of neutrons in the radiation field based on a ratio between the first value and the second value;
wherein the first value is based on a first depth profile for a luminescent material covered by a first converter comprising a first converter material that is exposed to the radiation field;
wherein the second value is based on a second depth profile for the luminescent material covered by a second converter comprising a second converter material that is exposed to the radiation field;
wherein the first and second converter materials are different from each other;
wherein the first and second depth profiles are each based on respective measurements of a respective set of one or more high spatial resolution fluorescence images of the luminescent material.
8. The method of claim 7 , wherein the first converter comprises a hydrogen-containing material and the second converter comprises a 6 Li isotope.
9. The method of claim 7 , wherein the method comprises the following step:
(c) determining the first and second values based on a spatial frequency domain analysis of the one or more high spatial resolution fluorescence images of the luminescent material.
10. A method comprising the following steps:
(a) providing a first value of a first power spectrum integral and a second value of a second power spectrum integral for a radiation field; and
(b) determining a median energy of neutrons in the radiation field based on a ratio between the first value and the second value;
wherein the first value is based on a first depth profile for a luminescent material covered by a first converter comprising a first converter material that is exposed to the radiation field;
wherein the second value is based on a second depth profile for the luminescent material covered by a second converter comprising a second converter material that is exposed to the radiation field;
wherein the first and second converter materials are different from each other; and
wherein the first and second depth profiles are each based on respective measurements of a respective set of one or more high spatial resolution fluorescence images of the luminescent material.
11. The method of claim 10 , wherein the first converter comprises a hydrogen-containing material and the second converter comprises a 6 Li isotope.
12. The method of claim 10 , wherein the method comprises the following step:
(c) determining the first and second values based on a spatial frequency domain analysis of the one or more high spatial resolution fluorescence images of the luminescent material.