Semiconductor Neutron Detection With Boron-10 Alpha-Ray Selection

Resolve Bottlenecks,
Find Innovative Solutions
Generate Solutions

Solution Overview

Problem

Semiconductor-based neutron detection elements exhibit output variation due to α-rays and Li-particle beams emitted in opposite directions, leading to inconsistent detection results.

Innovation Solution

A neutron detection element with a semiconductor layer and a neutron conversion layer containing boron 10 or lithium 6, which converts neutrons into α-rays and filters out Li-particle beams, using a configuration that only allows α-rays to generate electron-hole pairs for detection, with an amplifier to measure the output.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If both α-rays and Li-particle beams are detected in the depletion layer, then neutron detection capability is achieved, but output variation increases due to different charge generation amounts

Engineering Contradiction:
Improvedetection consistencyVSAvoidoutput variation
Core Design Contradiction:
ReliabilityVSMeasurement precision

Solution Approach 1:

The patent extracts only the α-ray detection function from the neutron conversion process by placing the 10B layer adjacent to the depletion layer, while Li-particle beams are emitted away from the depletion layer and not detected, thus eliminating output variation caused by detecting both particle types

Inventive Principle:
Principle #2Taking out (Extraction)

Solution Approach 2:

The patent creates a localized detection region by positioning the 10B-containing layer specifically adjacent to one side of the depletion layer, ensuring that only α-rays generated in this local region are detected, while Li-particle beams emitted in opposite directions are excluded from detection

Inventive Principle:
Principle #3Local quality

2Reliability

If a semiconductor-based neutron detection element is used, then neutron detection is achieved, but output variation occurs due to opposite direction emission of charged particles

Engineering Contradiction:
Improvedetection capabilityVSAvoidoutput consistency
Core Design Contradiction:
ReliabilityVSMeasurement precision

Solution Approach 1:

The patent introduces asymmetry in the detection geometry by placing the 10B layer adjacent to only one side of the depletion layer, creating an asymmetric configuration where α-rays are detected but Li-particle beams emitted in the opposite direction are not detected, thus achieving consistent output

Inventive Principle:
Principle #4Asymmetry

Data Source

PatentUS12416737B2Neutron detection element
Publication Date: 2025.09.16 HIROSHIMA UNIVERSITY
  • US12416737B2 patent drawing
  • US12416737B2 patent drawing
  • US12416737B2 patent drawing

AI summary

A neutron detection element 100 includes: a neutron detector configured to detect a neutron and convert the neutron into an electrical signal; and an amplifier configured to amplify an output of the neutron detector. The neutron detector includes: a semiconductor layer of a first conductivity type; a detector diffusion layer of a second conductivity type in the semiconductor layer; and a neutron conversion layer on the detector diffusion layer. The neutron conversion layer converts a neutron into an α-ray. The amplifier includes a plurality of transistors in the semiconductor layer. The neutron conversion layer is a metal film including a layer containing boron 10 or a layer containing lithium 6.