# US 2019/0170887 A1 · Antineutrino Detection Based on Heterogeneous Scintillation Lattice

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- Number: US 2019/0170887 A1
- Document ID: US20190170887A1
- Status: Published application
- Kind: A1
- Application number: 16/320,941
- Filed: 2016-10-21
- Published: 2019-06-06
- Earliest claimed: 2016-07-27
- Assignees: Virginia Tech Intellectual Properties, Inc.
- Applicants: Virginia Tech Intellectual Properties, Inc.
- Inventors: Patrick Huber; Jonathan M. Link; Mariani Camillo
- Web page: https://patentgrep.com/patent/US20190170887A1

## CPC

- G01T 3/06: with scintillation detectors
- G01T 1/1606: {with other specified detectors not provided for in the other subgroups of G01T1/16}
- 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 radiation detector and detection method comprising one or more antineutrino capture sections having a plurality of cells. The cells including hydrogen, act as scintillators and contain a wavelength shifter. Also included are a plurality of neutron capture layers containing a neutron capture agent. The cells are disposed between said neutron capture layers. The layers act as scintillators to convert the radiation emission of a neutron capture to light for transmission to at least one of the cells and the cells and layers have different scintillation time constants.

## Claims

### Claim 1

A radiation detector, comprising:
a plurality of antineutrino capture sections, said antineutrino capture sections comprised of a plurality of cells, said cells having planar surfaces and pairwise parallel surfaces;
said cells including hydrogen as a target for an antineutrino;
said cells act as scintillators and contain a wavelength shifter;
said pairwise parallel surfaces separated by a medium of a lower index of refraction;
a plurality of neutron capture sections containing a neutron capture agent that emits a radiation emission that remains within the neutron capture section upon the capture of a neutron;
said antineutrino capture sections disposed between said neutron capture sections;
said neutron capture sections act as scintillators to convert the radiation emission of a neutron capture to light for transmission to at least one of said cells; and
said cells and said neutron capture sections have different scintillation time constants.

### Claim 2 (depends on 1)

The detector of claim 1 wherein said pairwise parallel surfaces are separated by an air gap.

### Claim 3 (depends on 1)

The detector of claim 1 wherein said cells are in optical contact.

### Claim 4 (depends on 1)

The detector of claim 1 wherein said cells are cubes.

### Claim 5 (depends on 1)

The detector of claim 1 wherein said cells are cuboids.

### Claim 6 (depends on 1)

The detector of claim 1 wherein said cells have cross-sections that are triangular, quadrilateral or polygonal.

### Claim 7 (depends on 1)

The detector of claim 1 said scintillation time constant of said neutron capture sections is greater than the scintillation time constant of said antineutrino capture sections.

### Claim 8 (depends on 1)

The detector of claim 1 wherein said cells are optically connected to form axial channels in said antineutrino sections.

### Claim 9 (depends on 1)

The detector of claim 1 wherein light produced in said neutron capture sections is transmitted to one or more cells where it is absorbed and emitted isotropically by said wavelength shifter.

### Claim 10 (depends on 1)

The detector of claim 1 wherein light transmitted by said wavelength shifter of said neutron capture sections to said cells is emitted isotropically inside one or more cells and further axially transmitted by total internal reflection.

### Claim 11 (depends on 10)

The detector of claim 10 wherein light is transmitted along two or more channels.

### Claim 12

A radiation detector, comprising:
a plurality of antineutrino capture layers, said antineutrino capture layers comprised of a plurality of optically coupled cuboids, said cuboids having planar surfaces and pairwise parallel surfaces where said cuboids abut;
said cuboids including hydrogen as a target for antineutrinos;
said cuboids act as scintillators and contain a wavelength shifter;
said pairwise parallel surfaces separated by a medium of a lower index of refraction; a plurality of neutron capture layers adapted to emit a radiation emission that remains within the layers upon the capture of a neutron;
said antineutrino capture layers disposed between said neutron capture layers;
said neutron capture layers act as scintillators to convert the radiation emission of a neutron capture to light for transmission to at least one of said cuboids; and
said cuboids and said neutron capture layers have different scintillation time constants.

### Claim 13 (depends on 11)

The radiation detector of claim 11 wherein said cuboids have the same configuration.

### Claim 14 (depends on 11)

The detector of claim 11 wherein said cuboids are arranged to form axial channels in said antineutrino layers, one of said channels forming an x-axis and another channel forming a y-axis.

### Claim 15 (depends on 13)

The detector of claim 13 wherein light transmitted by said wavelength shifter of said antineutrino capture layers to said cuboids is emitted isotropically inside one or more cuboids and further axially transmitted along said x-axis and y-axis of said channels.

### Claim 16 (depends on 14)

The detector of claim 14 wherein said cuboids are arranged in optically isolated layers, said x-axis channels isolated by total internal reflection, and said y-axis channels isolated by total internal reflection.

### Claim 17 (depends on 11)

The detector of claim 11 wherein said cuboids are further arranged to reconstruct the angle formed by a primary positron and its annihilation γ-rays.

### Claim 18 (depends on 17)

The detector of claim 17 wherein the angle is reconstructed by using the cube that detects a primary positron to indicate the vertex of the angle and using the cubes that detect the annihilation γ-rays to indicate the side rays of the angle.

### Claim 19

A method for detecting an antineutrino event comprising the steps of:
creating an antineutrino capture event by providing a plurality of radiation capture layers to capture an antineutrino, said antineutrino event capture layers comprised of repeating optically coupled cells, said cells having planar surfaces and said cells have pairwise parallel surfaces where said cells abut;
said cells including hydrogen as target for capturing antineutrinos;
said cells act as scintillators and contain a wavelength shifter;
said pairwise parallel surfaces separated by a medium of a lower index of refraction;
creating a neutron capture event by providing a neutron capture medium containing a neutron capture agent for capturing a neutron, said neutron capture medium emits a radiation emission that remains within the capture medium upon the capture of a neutron; creating different light pulses of different duration for each capture event by adapting said cells and said neutron capture medium to have different scintillation time constants; and
scintillation light originating in said cells and said neutron capture medium is transmitted through the optically coupled cells along axial channels by total internal reflection where it is read out on the surface of the detector to provide x, y and z coordinates of the event.

### Claim 20 (depends on 19)

The method of claim 19 wherein said cells are segmented to determine the angle formed by a primary positron and its annihilation γ-rays

### Claim 21 (depends on 20)

The method of claim 20 wherein the angle is reconstructed by using the cell that detects a primary positron to indicate the vertex of the angle and using the cells that detect the annihilation γ-rays to indicate the side rays of the angle.