Electron Beam Microscope Layout for Backscatter Electron Detection

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Solution Overview

Problem

Conventional electron beam microscopes face inefficiencies in detecting backscatter electrons due to electrostatic fields that decelerate and misfocus the electron beam, leading to reduced detection efficiency of backscatter electrons compared to secondary electrons.

Innovation Solution

The electron beam microscope design includes a beam tube with variable potential settings and a scintillator arrangement within the objective lens, allowing for improved detection of backscatter electrons by decelerating the electron beam and generating light from electrons that enter the beam tube, which is then efficiently detected by a light detector system.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Manufacturing precision

If electrostatic fields are used to accelerate electrons and focus the electron beam, then the electron beam focusing is improved, but the detection efficiency of backscatter electrons deteriorates due to deceleration and misfocusing

Engineering Contradiction:
Improveelectron beam focusing precisionVSAvoidbackscatter electron detection efficiency
Core Design Contradiction:
Manufacturing precisionVSMeasurement precision

Solution Approach 1:

The detection system is segmented into multiple independent detectors positioned at different locations and angles. Secondary electron detectors are placed within the beam tube along the electron beam path, while backscatter electron detectors are positioned outside the beam tube at specific angles. This segmentation allows each detector to optimize its detection of specific electron types without interference from electrostatic fields that focus the primary beam.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The detection approach transitions from a single-dimension axial detection (along the beam axis) to multi-dimensional detection by placing detectors at various angular positions and locations. Backscatter electron detectors are positioned outside the beam tube at angles to detect electrons emerging in different directions, while secondary electron detectors are placed within the beam tube to catch electrons moving axially, thereby capturing backscatter electrons that would otherwise be misfocused by the electrostatic fields.

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

2Measurement precision

If a detector is arranged inside the beam tube to detect backscatter electrons, then the detection efficiency is improved, but the device complexity increases due to additional components and potential interference with the electron beam

Engineering Contradiction:
Improvebackscatter electron detection efficiencyVSAvoiddetector arrangement complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The detection system merges multiple detection functions into a coordinated arrangement where secondary electron detectors and backscatter electron detectors work together. The secondary electron detectors within the beam tube and backscatter electron detectors outside the beam tube are integrated into a unified detection system controlled by a single controller, reducing overall system complexity despite the multiple detector components.

Inventive Principle:
Principle #5Merging (Combining)

Solution Approach 2:

The beam tube itself serves as an intermediary structure that facilitates detection without requiring detectors to be placed directly in the electron beam path. The beam tube wall acts as a boundary that allows backscatter electrons to be detected from outside the tube while the secondary electron detectors inside the tube detect electrons that enter the beam tube, eliminating the need for complex internal detector arrangements that would directly interfere with the electron beam.

Inventive Principle:
Principle #24Intermediary (Mediator)

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 configuration enhances the detection efficiency of backscatter electrons by optimizing the electrostatic fields and positioning of the scintillator and detector arrangements, allowing for more accurate imaging of the object surface.

Implementation Method 1

Before the electrons enter the beam tube, they are accelerated to a high kinetic energy. The beam tube is an electrode which surrounds the electron beam and is at a given electric potential which is selected relative to the potential of the electron emitter of the electron beam source in such a way that the electrons entering the beam tube quickly cover the distance

Methodology Applied
Scientific EffectElectrostatic field: Electric Field

Implementation Method 2

The magnetic objective lens comprises a solenoid and a yoke with two pole ends, each extending around an axis of symmetry of the magnetic objective lens. Current flowing through the solenoid generates a magnetic field that exits the yoke at the pole ends and has a focusing effect on the electron beam

Methodology Applied
Scientific EffectMagnetic field: Magnetic Field

Implementation Method 3

The scintillator arrangement comprises a scintillator body, which generates light from electrons that are incident on the scintillator body and penetrate it, by converting part of the kinetic energy of the electrons into light

Methodology Applied
Scientific EffectScintillation: Scintillation

Implementation Method 4

The light is detected by a light detector of the detector arrangement in which, upon the incidence of light, generates electrical signals

Methodology Applied
Scientific EffectPhotoelectric effect: Photoelectric Effect

Data Source

PatentUS20240304410A1Electron beam microscope
Publication Date: 2024.09.12 CARL ZEISS MICROSCOPY GMBH
  • US20240304410A1 patent drawing
  • US20240304410A1 patent drawing
  • US20240304410A1 patent drawing

AI summary

An electron beam microscope comprises an electron beam source, a beam tube, a magnetic objective lens, an object holder, a scintillator arrangement, a detector arrangement and a potential supply system. The power supply system supplies: i) the object holder with a potential U1; ii) the beam tube with a potential U2; iii) a pole end of the objective lens with a potential U3; iv) a scintillator body of the scintillator arrangement with a potential; and v) a light detector of the detector arrangement with a potential U5, such that:(U⁢2-U⁢5)≥5000⁢ V;(U⁢4-U⁢1)≥0.1*(U⁢2-U⁢1)<semantics definitionURL="">❘<annotation encoding="Mathematica">"\[LeftBracketingBar]"</annotation></semantics>U⁢4-U⁢5<semantics definitionURL="">❘<annotation encoding="Mathematica">"\[RightBracketingBar]"</annotation></semantics>≥0.1*(U⁢2-U⁢1),and<semantics definitionURL="">❘<annotation encoding="Mathematica">"\[LeftBracketingBar]"</annotation></semantics>U⁢3-U⁢5<semantics definitionURL="">❘<annotation encoding="Mathematica">"\[RightBracketingBar]"</annotation></semantics>≤0.3*(U⁢2-U⁢1).