Liquid-Jet X-Ray Source Debris Reduction via Focused Electron Beam

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Solution Overview

Problem

Current compact electron-impact x-ray sources are limited by thermal effects, restricting the brightness and power density of the x-ray source, and the use of liquid-jet anodes faces challenges with debris emission when attempting to increase power density.

Innovation Solution

Employing an electron beam with a full width at half maximum (FWHM) that is about half the transverse dimension of the target jet or less, which creates a shielding effect to reduce debris and increase effective power density by focusing the electron beam to a smaller size compared to the target jet, allowing for higher thermal load without increasing jet speed.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Illumination intensity

If the electron beam spot size is reduced to increase power density, then x-ray brightness is improved, but debris emission increases

Engineering Contradiction:
Improvex-ray brightnessVSAvoiddebris emission
Core Design Contradiction:
Illumination intensityVSObject-generated harmful factors

Solution Approach 1:

The patent applies local quality by creating a temperature gradient across the target jet cross-section, with the center region (where the electron beam impacts) being hottest and the periphery being cooler. This spatial variation in temperature allows the hot central region to generate high x-ray brightness while the cooler peripheral regions suppress debris emission, effectively decoupling these two previously conflicting requirements.

Inventive Principle:
Principle #3Local quality

2Object-generated harmful factors

If the liquid jet transverse dimension is reduced to maintain shielding effect, then debris is reduced, but the target area for x-ray generation is limited

Engineering Contradiction:
Improvedebris emissionVSAvoidtarget area
Core Design Contradiction:
Object-generated harmful factorsVSArea of stationary object

Solution Approach 1:

The patent resolves this contradiction by transitioning from a two-dimensional area constraint to a three-dimensional volume utilization. The electron beam is focused to a small spot size (maintaining the shielding effect) but can be positioned at multiple locations along the length of the liquid jet. This allows the system to maintain a small interaction cross-section (reducing debris) while utilizing the full volume of the liquid jet target (maintaining or increasing total x-ray generation area).

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 significantly reduces debris production and enhances x-ray brightness by maintaining high power density while minimizing thermal limitations, enabling increased x-ray production without the need for extreme jet speeds.

Implementation Method 1

As the electrons impact the target they lose energy in one of two ways: either they can be decelerated in the electric field close to an atomic nucleus and emit continuous bremsstrahlung radiation

Methodology Applied
Scientific EffectBremsstrahlung radiation:

Implementation Method 2

or they can knock out an inner-shell electron, resulting in the emission of a characteristic x-ray photon when the vacancy is filled

Methodology Applied
Scientific EffectCharacteristic x-ray emission:

Implementation Method 3

The brightness of current state-of-the-art compact electron-impact x-ray sources is limited by thermal effects in the anode

Methodology Applied
Scientific EffectThermal conduction: Conduction (thermal)

Data Source

PatentEP2016608B1Method and system of debris reduction in electron-impact x-ray sources
Publication Date: 2016.08.17 JETTEC AB
  • EP2016608B1 patent drawingFigure 1
  • EP2016608B1 patent drawingFigure 2~3
  • EP2016608B1 patent drawing

AI summary

A method for generating x-ray radiation, comprising the steps of forming a target jet by urging a liquid substance under pressure through an outlet opening, the target jet propagating through an area of interaction; and directing at least one electron beam onto the target jet in the area of interaction such that the electron beam interacts with the target jet to generate x-ray radiation; wherein the full width at half maximum of the electron beam in the transverse direction of the target jet is about 50% or less of the target jet transverse dimension. A system for carrying out the method is also disclosed.