# US 2014/0077085 A1 · Radiation Detector Having a Ribbed Scintillator > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 2014/0077085 A1 - Document ID: US20140077085A1 - Status: Published application - Kind: A1 - Application number: 14/089,352 - Filed: 2013-11-25 - Published: 2014-03-20 - Earliest claimed: 2010-09-13 - Assignees: PartTec, Ltd. - Inventors: Herschel Ellis Workman; Craig R. Kline - Web page: https://patentgrep.com/patent/US20140077085A1 ## CPC - G01T 3/06: with scintillation detectors - G01T 5/08: Scintillation chambers (discharge tubes H01J40/00, H01J47/00) - Y10T 29/49826: Assembling or joining - 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) - Y10T: TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION ## Abstract A system for efficient neutron detection is described. The system includes a neutron scintillator formed with a number of protruding parallel ribs each side of the scintillator, forming a first set of ribs and a second set of ribs. The ribs have a protrusion height that provides a selected neutron absorption efficiency. The system includes a set of wavelength shifting fibers positioned between each adjacent pair of ribs on both the first side and the second side. Each set of wavelength shifting fibers are in optical proximity to the adjacent pair of the ribs that set of fibers are positioned between. ## Claims ### Claim 1 A method, comprising: determining a neutron absorption efficiency per linear distance through a selected neutron scintillator material; determining a desired neutron absorption efficiency for a neutron detector; determining a neutron mean absorption distance in response to the neutron absorption efficiency and the desired neutron absorption efficiency; and providing a neutron scintillator comprising the selected neutron scintillator material, the neutron scintillator formed with a multiplicity of protruding parallel ribs on a first side (first ribs) and a second multiplicity of protruding parallel ribs on a second side (second ribs), wherein each of the first ribs and the second ribs comprises a protrusion height at least equal to the neutron mean absorption distance, wherein the neutron scintillator is at least locally planar, and wherein the first ribs are offset from the second ribs such that a particle passing through the neutron scintillator perpendicular to the neutron scintillator plane must either pass through at least one rib from the first ribs or at least one rib from the second ribs; and further providing a set of wavelength shifting fibers positioned between each adjacent pair of the first ribs and each adjacent pair of the second ribs, wherein each set of wavelength shifting fibers is in optical proximity to the adjacent pair of the ribs that set of the wavelength shifting fiber is positioned between, and wherein each set of wavelength shifting fibers comprises a sufficient number of fibers to optically cover the adjacent pair of the ribs to a height of at least the neutron mean absorption distance. ### Claim 2 (depends on 1) The method of claim 1, wherein providing the neutron scintillator further comprises providing the neutron scintillator comprising at least one material selected from the materials consisting of: 6Li, 10B, 6LiF:ZnS/Ag, a P47 phosphor, and (6LiF:Y2SiO5:Ce). ### Claim 3 (depends on 2) The method of claim 2, further comprising determining the desired neutron absorption efficiency to be at least 30% absorption of incident neutrons. ### Claim 4 (depends on 2) The method of claim 2, further comprising determining the desired neutron absorption efficiency to be at least 50% absorption of incident neutrons. ### Claim 5 (depends on 2) The method of claim 2, further comprising determining the desired neutron absorption efficiency to be at least 80% absorption of incident neutrons. ### Claim 6 (depends on 2) The method of claim 2, further comprising determining the neutron absorption efficiency to be about 83% absorption of incident neutrons. ### Claim 7 (depends on 1) The method of claim 1, further comprising: determining a plurality of electrical signals in response to light emissions from the set of wavelength shifting fibers positioned between each adjacent pair of the first ribs and each adjacent pair of the second ribs; wherein the determining the plurality of electrical signals comprises determining distinct electrical signals from any two adjacent wavelength shifting fibers; and distinguishing a neutron radiation event from a gamma radiation event in response to two adjacent wavelength shifting fibers providing simultaneous electrical signals. ### Claim 8 (depends on 18) The method of claim 18, wherein the protrusion height of the first ribs and the protrusion height of the second ribs are formed by stacking a plurality of scintillator body portions. ### Claim 9 A method, comprising: determining a neutron absorption efficiency per linear distance through a selected neutron scintillator material; determining a desired neutron absorption efficiency for a neutron detector; determining a neutron mean absorption distance in response to the neutron absorption efficiency and the desired neutron absorption efficiency; and providing a neutron scintillator comprising the selected neutron scintillator material, the neutron scintillator formed with a multiplicity of protruding parallel ribs on a first side (first ribs) and a second multiplicity of protruding parallel ribs on a second side (second ribs), wherein each of the first ribs and the second ribs comprises a protrusion height at least equal to the neutron mean absorption distance, and wherein the first ribs are offset from the second ribs such that a particle passing through the neutron scintillator perpendicular to the neutron scintillator plane must either pass through at least one rib from the first ribs or at least one rib from the second ribs; and further providing a set of wavelength shifting fibers positioned between each adjacent pair of the first ribs and each adjacent pair of the second ribs, and wherein each set of wavelength shifting fibers comprises a sufficient number of fibers to optically cover the adjacent pair of the ribs to a height of at least the neutron mean absorption distance. ### Claim 10 (depends on 9) The method of claim 9, wherein the neutron scintillator is at least locally planar. ### Claim 11 (depends on 9) The method of claim 9, further comprising the step of directing each set of wavelength shifting fibers to at least a first light converter and a second light converter. ### Claim 12 (depends on 11) The method of claim 11, wherein alternating fibers in said set of wavelength shifting fibers positioned between said ribs is directed to said first light converter and all others are directed to said second light converter. ### Claim 13 A method, comprising: providing a scintillator body having an upper portion and a lower portion, wherein said upper portion includes a first plurality of ribs protruding upwardly, wherein said first plurality of ribs are generally parallel to one another, wherein said lower portion includes a second plurality of ribs protruding downwardly, wherein said second plurality of ribs are generally parallel to one another; placing at least two or more wavelength shifting fibers in a stacked relationship to one another in a plurality of slots defined between at least two ribs in said upper and lower portion such that a plurality of wavelength shifting fibers are positioned between ribs in said first plurality of ribs and said second plurality of ribs; and directing an end of said plurality of wavelength shifting fibers to at least one of two light converters, wherein ends of adjacent wavelength shifting fibers between respective ribs are not directed to the same light converter. ### Claim 14 (depends on 13) The method of claim 13, wherein a ratio of wavelength shifting fibers to light converters comprises from about 1:1 to 100:1. ### Claim 16 (depends on 13) The method of claim 13, further comprising connecting said light converters to a controller configured to monitor neutron detection events. ### Claim 17 (depends on 13) The method of claim 13, wherein said ribs have a thickness in the range of about 0.2 mm to 1.0 mm. ### Claim 18 (depends on 17) The method of claim 17, wherein said wavelength shifting fibers have an outside diameter of about 0.2 mm to 0.3 mm. ### Claim 19 (depends on 13) The method of claim 13, wherein each of the ribs comprises a protrusion height at least equal to a neutron mean absorption distance. ### Claim 20 (depends on 13) The method of claim 13, wherein said scintillator body has a generally cylindrical shape.