Charged Particle Detector With Conversion Surface
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Solution Overview
Problem
Conventional charged particle detectors face challenges such as saturation and damage from high transmitted charged particle currents, inefficiency, and high costs, making it difficult to effectively detect transmitted charged particles in transmission microscopy.
Innovation Solution
The development of charged particle detectors that generate secondary electrons by converting transmitted particles into a plurality of secondary electrons, using materials with high secondary electron yields and tilting conversion surfaces to increase conversion factors, allowing for efficient detection without saturation and integration with conventional detectors for robust systems.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Reliability
If conventional charged particle detectors are used to detect transmitted particles, then detection capability is provided, but the detectors saturate and are damaged by high transmitted charged particle currents
Solution Approach 1:
The patent introduces a conversion surface as an intermediary between the transmitted charged particles and the detector. The conversion surface converts incident charged particles into secondary electrons, which then strike the detector. This intermediary protects the detector from direct exposure to high particle currents that would cause saturation and damage, while still enabling efficient detection through the secondary electron conversion process.
2Productivity
If conversion surfaces are tilted to increase conversion factor, then detection efficiency is improved, but device complexity increases
Solution Approach 1:
The patent modifies the geometric parameter of the conversion surface by tilting it at a specific angle (e.g., 45 degrees) relative to the incident particle direction. This parameter change increases the conversion factor from approximately 1 secondary electron per incident particle at normal incidence to approximately 2 secondary electrons per incident particle at 45-degree incidence. The tilted configuration is integrated into the detector structure with appropriate spacing, achieving enhanced detection efficiency without excessive complexity.
3Productivity
If materials with higher secondary electron yields are used, then conversion factor is increased, but manufacturing complexity and cost increase
Solution Approach 1:
The patent changes the material parameter of the conversion surface by selecting materials with high secondary electron yield (SEY), such as platinum, tungsten, or tungsten alloys. These materials can produce 2 or more secondary electrons per incident charged particle, significantly improving the conversion factor. The patent balances manufacturing considerations by providing alternative materials like aluminum or stainless steel that offer lower but still acceptable SEY values, allowing selection based on specific application requirements and manufacturing capabilities.
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
These detectors provide efficient and reliable detection of transmitted charged particles, enabling the generation of sample images with various contrast mechanisms and enhancing information on sample characteristics like thickness, crystalline structure, and elemental composition without saturating or being damaged by high particle currents.
Implementation Method 1
a first material layer positioned on a first surface of a support structure and configured to generate secondary electrons in response to incident charged particles that strike the first layer
Implementation Method 2
the second layer being configured to generate secondary electrons in response to charged particles that pass through the aperture and strike the second layer
Data Source
AI summary
Disclosed are devices, systems, and methods are disclosed that include: (a) a first material layer positioned on a first surface of a support structure and configured to generate secondary electrons in response to incident charged particles that strike the first layer, the first layer including an aperture configured to permit a portion of the incident charged particles to pass through the aperture; and (b) a second material layer positioned on a second surface of the support structure and separated from the first layer by a distance of 0.5 cm or more, the second layer being configured to generate secondary electrons in response to charged particles that pass through the aperture and strike the second layer, where the device is a charged particle detector.


