Detection of nitrogenous material
First Claim
1. A method for the detection of nitrogenous materials or assaying of nitrogenous concentrations within an object, comprising:
- (i) placing on one side of the object a target containing 13 C for bombardment with 1.75 MeV protons to produce a source of 9.17 MeV γ
-rays;
(ii) placing on the opposite side of the object a γ
-ray detector or array of detectors with a nitrogen rich detection medium;
(iii) scanning the object with γ
-ray beam from said source;
(iv) reading from said γ
-ray detector or array of detectors the total and the non-resonant attenuations of the incident photon flux; and
(v) deriving from said attenuations the net resonant attenuation and the spatial distribution thereof;
characterized in that the said target is a member of the group consisting of 13 C pellets at least 25μ
thick and bodies bearing at least one composite thin film being not more than 1μ
thick and including at least one 13 C layer and at least one other layer, said at least one other layer containing a substance that is capable of generating supplementary γ
-radiation for determining the non-resonant component of attenuation.
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Accused Products
Abstract
Improved method and means for the detection of nitrogenous material or assaying of nitrogenous material in an object on the basis of nuclear resonant attenuation of 9.17 MeV γ-rays. A target in form of one or several 13 C pellets at least 25μ thick, or alternatively in form of a body that bears a composite thin film including at least one 13 C layer not more than 1μ thick and at least one other substance that is capable of generating supplementary γ-radiation for determining the non-resonant component of attenuation, is bombarded with 1.75 MeV protons to produce a source of 9.17 MeV γ-rays. The target is placed on one side of the inspected object and a γ-ray detector or an array of such detectors is placed on the other side and the total and non-resonant attenuation are read and evaluated.
45 Citations
13 Claims
-
1. A method for the detection of nitrogenous materials or assaying of nitrogenous concentrations within an object, comprising:
-
(i) placing on one side of the object a target containing 13 C for bombardment with 1.75 MeV protons to produce a source of 9.17 MeV γ
-rays;(ii) placing on the opposite side of the object a γ
-ray detector or array of detectors with a nitrogen rich detection medium;(iii) scanning the object with γ
-ray beam from said source;(iv) reading from said γ
-ray detector or array of detectors the total and the non-resonant attenuations of the incident photon flux; and(v) deriving from said attenuations the net resonant attenuation and the spatial distribution thereof; characterized in that the said target is a member of the group consisting of 13 C pellets at least 25μ
thick and bodies bearing at least one composite thin film being not more than 1μ
thick and including at least one 13 C layer and at least one other layer, said at least one other layer containing a substance that is capable of generating supplementary γ
-radiation for determining the non-resonant component of attenuation. - View Dependent Claims (2, 3, 4, 5, 6)
-
-
7. 13 C pellets which are at least 25μ
- thick for use as targets for bombardment with 1.75 MeV protons for the generation of 9.17 MeV γ
-rays and supplementary radiation for determining the non-resonant component of attenuation. - View Dependent Claims (8, 9, 10)
- thick for use as targets for bombardment with 1.75 MeV protons for the generation of 9.17 MeV γ
-
11. A target for bombardment with 1.75 MeV protons for the generation of 9.17 MeV γ
- -rays, comprising a body bearing a composite thin film not more than 1μ
thick and including at least one 13 C layer and at least one other layer containing a substance capable of generating supplementary radiation for determining the non-resonant component of attenuation. - View Dependent Claims (12, 13)
- -rays, comprising a body bearing a composite thin film not more than 1μ
Specification