# US 10,371,837 B2 · Directional neutron detector

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- Number: US 10,371,837 B2
- Document ID: US10371837B2
- Status: Granted
- Kind: B2
- Application number: 15/477,083
- Filed: 2017-04-01
- Published: 2018-06-21
- Granted: 2019-08-06
- Earliest claimed: 2016-12-19
- Applicants: David Edward Newman
- Inventors: David Edward Newman
- Web page: https://patentgrep.com/patent/US10371837B2

## CPC

- G01T 3/06: with scintillation detectors
- G01T: MEASUREMENT OF NUCLEAR OR X-RADIATION (radiation analysis of materials, mass spectrometry G01N23/00; tubes for determining the presence, intensity, density or energy of radiation or particles H01J47/00)

## Abstract

A neutron detector that indicates the direction toward a neutron source. The detector is a proton-recoil type of detector, in which two different scintillators are positioned on both sides of a hydrogenous target. Proton recoil signals from the two scintillators indicate whether neutrons arrive from the left, right, or center relative to the detector alignment. Surprisingly high precision can be obtained by orienting the detector so that the counting rates in the two scintillators are equal, at which point the target layer is directly aligned with the source. Disclosed are thick and thin target configurations, versions for discriminating pulses from the two scintillators, options for assembling a multi-detector stack and array, and multiple analysis procedures for optimally locating the neutron source.

## Claims

### Claim 1

A device comprising:
a target comprising a substantially planar layer of hydrogenous material that emits a recoil proton responsive to a neutron scattering event therein;
a first scintillator comprising a substantially planar layer of material that emits a first light pulse responsive to traversal by a charged particle;
a second scintillator comprising a substantially planar layer of material that emits a second light pulse responsive to traversal by a charged particle;
a discrimination module for determining whether a received light pulse is a first light pulse or a second light pulse; and
a counting module for storing a first count of the number of first light pulses received by the discrimination module, and a second count of the number of second light pulses received by the discrimination module, the difference between the first count and the second count indicating a direction of a neutron source relative to the device along an axis that is orthogonal to both substantially planar layers of the first and second scintillators;
wherein:
the first scintillator layer and the second scintillator layer are each configured to receive a recoil proton from the target layer;
the first scintillator layer and the second scintillator layer are substantially parallel to each other;
the first scintillator layer is proximate to a first side of the target layer; and
the second scintillator layer is proximate to a second side of the target layer, the second side being opposite to the first side of the target layer.

### Claim 2 (depends on 1)

The device of claim 1, wherein the first scintillator material is non-hydrogenous and the second scintillator material is non-hydrogenous.

### Claim 3 (depends on 1)

The device of claim 1, further comprising a second target of hydrogenous material wherein:
the first scintillator is proximate to the target of claim 1; and
the second scintillator is proximate to the second target.

### Claim 4 (depends on 1)

The device of claim 1, wherein the target comprises a non-scintillating material.

### Claim 5 (depends on 1)

The device of claim 1, wherein the target comprises a material that emits a third light pulse, different from the first and second light pulses, when traversed by a charged particle.

### Claim 6 (depends on 1)

The device of claim 1, further comprising:
one or more light guides, each light guide comprising a substantially planar body of non-hydrogenous transparent material optically coupled to at least one of the scintillators; and
one or more light sensors, each light sensor comprising a transducer, configured to generate an electrical pulse responsive to receiving a light pulse, each light sensor being optically coupled to at least one of the light guides.

### Claim 7 (depends on 1)

The device of claim 1, wherein:
the first scintillator layer has a thickness related to the stopping range of the recoil proton therein; and
the second scintillator layer has a thickness related to the stopping range of the recoil proton therein.

### Claim 8 (depends on 1)

The device of claim 1, wherein the target layer has a thickness related to the stopping range of the recoil proton therein.

### Claim 9 (depends on 1)

The device of claim 1, wherein:
the first light pulse has a first shape or duration; and
the second light pulse has a second shape or duration, different from the first shape or duration.

### Claim 10 (depends on 1)

The device of claim 1, wherein:
the first light pulse has a first wavelength; and
the second light pulse has a second wavelength, different from the first wavelength.

### Claim 11 (depends on 10)

The device of claim 10, further comprising:
a first optical filter that transmits the first wavelength and blocks or reflects the second wavelength; and
a second optical filter that transmits the second wavelength and blocks or reflects the first wavelength.

### Claim 12 (depends on 1)

The device of claim 1, further comprising a layer of reflective material between the target layer and one of the scintillator layers.

### Claim 13 (depends on 1)

The device of claim 1, further comprising:
a first light guide optically coupled to the first scintillator; and
a second light guide optically coupled to the second scintillator.

### Claim 14 (depends on 13)

The device of claim 13, further comprising a barrier of opaque material configured to optically isolate the first and second light guides from each other.

### Claim 15

A system comprising:
a plurality of targets, each target comprising a substantially planar layer of hydrogenous material configured to emit a recoil proton responsive to a neutron scattering event therein;
a plurality of first scintillators, each first scintillator comprising a substantially planar layer of non-hydrogenous material that emits a first light pulse responsive to traversal by a charged particle;
a plurality of second scintillators, each second scintillator comprising a substantially planar layer of non-hydrogenous material that emits a second light pulse responsive to traversal by a charged particle, the first and second light pulses being detectably different from each other;
wherein:
each first scintillator and each second scintillator are configured to receive a recoil proton from a respective target;
each target has a first side and a second side which is opposite to the first side;
each first scintillator is proximate to the first side of a target;
each second scintillator is proximate to the second side of a target; and
the first light pulse signals that a neutron source is located in a first region, and the second light pulse signals that a neutron source is located in a second region, wherein the first and second regions are separated by a plane parallel to and centered between said substantially planar layers of hydrogenous material.

### Claim 16 (depends on 15)

The system of claim 15, further comprising:
a plurality of light guides, each light guide comprising a transparent non-hydrogenous material; and
one or more light sensors, each light sensor comprising a transducer that generates an electronic signal responsive to a light pulse;
wherein:
each scintillator is optically coupled to exactly one of the light guides;
each light guide is optically coupled to one or two of the scintillators;
each light guide is optically coupled to at least one of the light sensors; and
each light sensor is optically coupled to at least one of the light guides.

### Claim 17 (depends on 15)

The system of claim 15, further comprising a plurality of opaque layers configured to optically isolate the first and second scintillators from each other.