Layered Semiconductor Scintillator for High-Energy Radiation Detection

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Solution Overview

Problem

Existing scintillators face challenges in achieving high energy resolution due to nonlinear processes and attenuation of luminescence in wide-gap insulating materials, while semiconductor scintillators struggle with transparency issues, limiting the efficiency of photon delivery to the surface.

Innovation Solution

A layered semiconductor heterostructure with wide-gap barrier regions and narrow-gap well regions, where minority carriers recombine radiatively in the barriers and generate scintillating photons that are efficiently captured by the wells, allowing for longer well separation and increased transparency, and utilizing high radiative efficiency to minimize signal loss through photon recycling.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Illumination intensity

If heavily doped semiconductor is used to shift absorption edge (Burstein shift), then transparency to scintillation radiation is improved, but attenuation of signal still occurs and depends on interaction depth

Engineering Contradiction:
Improvetransparency to scintillation radiationVSAvoidsignal attenuation
Core Design Contradiction:
Illumination intensityVSLoss of energy

Solution Approach 1:

The semiconductor crystal is divided into a layered heterostructure with alternating wide-gap barrier layers and narrow-gap well layers. The well layers are positioned at specific depths to capture scintillation photons generated in the barrier layers, enabling efficient photon collection from deep interaction sites while maintaining overall structural integrity and function.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The narrow-gap well layers act as intermediary structures that absorb scintillation photons generated in the wide-gap barrier layers and re-emit them at longer wavelengths. This intermediary mechanism enables photons generated deep within the semiconductor to be captured and re-transmitted, overcoming the attenuation problem without requiring heavy doping.

Inventive Principle:
Principle #24Intermediary (Mediator)

2Illumination intensity

If wide-gap insulating materials are used for scintillators, then self-luminescence transparency is improved, but carrier transport efficiency deteriorates due to poor mobility

Engineering Contradiction:
Improveself-luminescence transparencyVSAvoidcarrier transport efficiency
Core Design Contradiction:
Illumination intensityVSProductivity

Solution Approach 1:

Different regions of the semiconductor structure have different gap sizes optimized for specific functions: wide-gap barrier layers provide transparency to scintillation radiation and generate efficient scintillation, while narrow-gap well layers provide efficient carrier transport and photon capture. This local differentiation resolves the contradiction between transparency and transport efficiency.

Inventive Principle:
Principle #3Local quality

Solution Approach 2:

The scintillator uses a composite layered structure combining wide-gap and narrow-gap semiconductor materials. The wide-gap materials (e.g., GaN, AlGaN) provide transparency and scintillation generation, while the narrow-gap materials (e.g., InGaN, InAlGaN) provide efficient carrier transport and photon absorption, creating a composite system that achieves both requirements simultaneously.

Inventive Principle:
Principle #40Composite materials

3Volume of stationary object

If thicker scintillator structures are used to increase detection volume, then detection efficiency is improved, but signal attenuation increases

Engineering Contradiction:
Improvescintillator detection volumeVSAvoidsignal attenuation
Core Design Contradiction:
Volume of stationary objectVSLoss of energy

Solution Approach 1:

The thick scintillator structure is segmented into multiple alternating layers of wide-gap and narrow-gap materials. The narrow-gap well layers are strategically positioned throughout the thickness to capture photons generated at various depths, ensuring that even photons from deep interactions are collected efficiently, thus enabling thick structures without proportionally increased attenuation.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The solution transitions from a homogeneous one-dimensional structure to a multi-layered structure with periodic variation in material properties. This dimensional complexity allows photons to be captured at multiple depths and wavelengths, effectively decoupling the detection volume from signal attenuation and enabling thick detectors with high efficiency.

Inventive Principle:
Principle #17Another dimension (Dimensionality change)

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

This approach enhances energy resolution by ensuring efficient capture and transmission of scintillating photons, reducing attenuation, and allowing for thicker scintillator structures without significant loss of signal, thereby improving the detection efficiency of high-energy radiation.

Implementation Method 1

minority carriers recombine radiatively in the barriers and generate scintillating photons

Methodology Applied
Scientific EffectRadiative recombination: Luminescence

Implementation Method 2

efficiently captured by the wells

Methodology Applied
Scientific EffectOptical absorption: Absorption (EM radiation)

Data Source

PatentUS8664612B2Layered semiconductor scintillator
Publication Date: 2014.03.04 THE RES FOUNDATION FOR THE STATE UNIV OF NEW YORK
  • US8664612B2 patent drawing
  • US8664612B2 patent drawing
  • US8664612B2 patent drawing

AI summary

A scintillator detector of high-energy radiation comprising a semiconductor slab that is composed of alternating layers of barrier and well material. The barrier and well material layers are direct bandgap semiconductors. Bandgap of the well material is smaller than the bandgap of the barrier material. The combined thickness of the well layers is substantially less than the total thickness of said slab. The thickness of the barrier layers is substantially larger than the diffusion length of minority carriers. The thickness of the well layers is sufficiently large to absorb most of the incident scintillating radiation generated in the barrier layers in response to an ionization event from interaction with an incident high-energy particle.