High Radiance X-Ray Source Using Electron Emitter Array

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Solution Overview

Problem

Current x-ray sources in semiconductor metrology face challenges in achieving high radiance, which is necessary for accurately measuring small dimensions and defects in advanced semiconductor structures due to limitations in electron beam power conversion and anode material durability.

Innovation Solution

A high radiance x-ray source is developed using a high density electron emitter array with a large electron current focused onto a small anode area, featuring an array of electron emitters with high current density and controlled extractor voltage channels, and an optical light source to enhance electron emission, maintaining the electron emitter array in a vacuum environment with a pressure differential to prevent gas flow and heat dissipation.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If a traditional x-ray source with limited electron beam power is used, then the device complexity is reduced, but the radiance and measurement precision deteriorate

Engineering Contradiction:
Improvemeasurement precisionVSAvoiddevice complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The electron emitter is divided into an array of multiple individual emitters (e.g., 10x10 grid) rather than using a single emitter. Each emitter can be independently controlled, allowing the system to achieve high radiance through collective emission while maintaining manageable complexity through modular architecture

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent transitions from a single-point electron emitter to a two-dimensional array of emitters, adding spatial dimensionality to the electron source. This dimensional expansion enables high radiance by distributing electron emission across multiple points while focusing the combined beam on a small anode area

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

2Power

If electron beam power is increased to achieve high radiance, then the radiance improves, but the anode material durability deteriorates

Engineering Contradiction:
ImproveradianceVSAvoidanode material durability
Core Design Contradiction:
PowerVSReliability

Solution Approach 1:

The total electron beam power is segmented across multiple individual emitters in the array, distributing the thermal and mechanical stress on the anode. This segmentation allows high total power delivery while preventing localized overheating and material degradation

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent changes the operational parameters by using many low-power emitters instead of one high-power emitter, altering the power distribution characteristics. This parameter change enables high radiance while maintaining anode durability through reduced peak power density

Inventive Principle:
Principle #35Parameter changes

3Measurement precision

If optical radiation is used for metrology, then the ease of operation is improved, but the measurement precision deteriorates for nanometer-scale structures

Engineering Contradiction:
Improvemeasurement precisionVSAvoiddevice complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent replaces optical radiation with x-ray radiation generated by electron bombardment. This substitution enables precise measurement of nanometer-scale and sub-nanometer structures by using x-rays with wavelengths much shorter than visible or UV light, overcoming the diffraction limits of optical systems

Inventive Principle:
Principle #28Mechanics substitution (Replace mechanical system)

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 solution enables high throughput x-ray metrology and inspection with improved penetration and sensitivity, allowing for precise measurement of structural and material characteristics in semiconductor fabrication processes, overcoming limitations of traditional x-ray sources.

Implementation Method 1

an array of electron emitters with high current density

Methodology Applied
Scientific EffectField emission: Electron Paramagnetic Resonance

Implementation Method 2

an optical light source to enhance electron emission

Methodology Applied
Scientific EffectThermionic emission: Thermionic Emission

Implementation Method 3

electrons emitted by the array of electron emitters are accelerated from the electron emitter array to the anode

Methodology Applied
Scientific EffectElectrostatic acceleration: Electrostatics

Implementation Method 4

the incidence of the electron current flow onto the anode structure stimulates x-ray emission

Methodology Applied
Scientific EffectBremsstrahlung radiation:

Implementation Method 5

a desired characteristic x-ray wavelength

Methodology Applied
Scientific EffectCharacteristic x-ray emission:

Implementation Method 6

maintaining the electron emitter array in a vacuum environment with a pressure differential to prevent gas flow and heat dissipation

Methodology Applied
Scientific EffectVacuum: Vacuum

Data Source

PatentUS11719652B2Semiconductor metrology and inspection based on an x-ray source with an electron emitter array
Publication Date: 2023.08.08 KLA CORP
  • US11719652B2 patent drawing
  • US11719652B2 patent drawing
  • US11719652B2 patent drawing

AI summary

Methods and systems for realizing a high radiance x-ray source based on a high density electron emitter array are presented herein. The high radiance x-ray source is suitable for high throughput x-ray metrology and inspection in a semiconductor fabrication environment. The high radiance X-ray source includes an array of electron emitters that generate a large electron current focused over a small anode area to generate high radiance X-ray illumination light. In some embodiments, electron current density across the surface of the electron emitter array is at least 0.01 Amperes/mm2, the electron current is focused onto an anode area with a dimension of maximum extent less than 100 micrometers, and the spacing between emitters is less than 5 micrometers. In another aspect, emitted electrons are accelerated from the array to the anode with a landing energy less than four times the energy of a desired X-ray emission line.