X-Ray Fluorescence Spectrometer Counting Loss Precision Correction

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Solution Overview

Problem

Conventional X-ray fluorescence spectrometers underestimate the fluctuation in counting loss correction, leading to overestimation of counting precision at high fluorescent X-ray intensities, resulting in inaccurate quantitative analysis.

Innovation Solution

An X-ray fluorescence spectrometer that calculates and displays the theoretical standard deviation of corrected differential intensity using equation (1), reflecting fluctuations in counting loss correction, and determines an optimal tube current value for precise analysis.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If conventional counting precision estimation methods are used, then calculation simplicity is maintained, but measurement precision deteriorates due to overestimation of counting precision at high intensities

Engineering Contradiction:
Improvecounting precisionVSAvoidcalculation complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent changes the parameters used in counting precision estimation from simple uncorrected intensity values to corrected intensity values that account for counting loss. Specifically, it uses corrected differential intensity (Iw) and corrected integrated intensity (It) along with their respective counting loss correction coefficients (τw and τd) to calculate theoretical standard deviation, thereby improving measurement precision while managing calculation complexity through systematic parameter transformation.

Inventive Principle:
Principle #35Parameter changes

2Productivity

If high-intensity fluorescent X-rays are measured, then productivity increases, but measurement precision deteriorates due to significant counting loss

Engineering Contradiction:
Improvemeasurement throughputVSAvoidcounting precision
Core Design Contradiction:
ProductivityVSMeasurement precision

Solution Approach 1:

The patent implements a feedback mechanism where the measured uncorrected intensities (Iw0 and It0) are used to calculate the counting loss correction coefficients (τw and τd), which then feed back into the corrected intensity calculation. This closed-loop approach allows the system to automatically compensate for counting loss effects, enabling high-intensity measurements to maintain precision while improving productivity through faster counting rates.

Inventive Principle:
Principle #23Feedback

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

Enables accurate quantitative analysis with appropriate counting precision by accounting for counting loss fluctuations, reducing the standard deviation by 11% compared to conventional methods.

Implementation Method 1

an X-ray fluorescence spectrometer which irradiates a sample with primary X-rays from an X-ray tube and which performs, based on intensities of generated fluorescent X-rays

Methodology Applied
Scientific EffectX-ray fluorescence: Fluorescence

Data Source

PatentEP4707788A1X-ray fluorescence spectrometer
Publication Date: 2026.03.11 RIGAKU CORP
  • EP4707788A1 patent drawingFigure 1
  • EP4707788A1 patent drawing
  • EP4707788A1 patent drawing

AI summary

In an X-ray fluorescence spectrometer of the present invention, a quantification unit calculates a theoretical standard deviation of a corrected differential intensity as counting precision, based on an uncorrected integrated intensity and an uncorrected differential intensity, by equation (1), and displays the theoretical standard deviation. σWIt0,IW0=∂IW/∂It02⋅σIt02+∂IW/∂IW02⋅σIW021/2 where, σW: theoretical standard deviation of corrected differential intensity, It0: uncorrected integrated intensity, Iw0: uncorrected differential intensity, IW: corrected differential intensity, σIt0: theoretical standard deviation of uncorrected integrated intensity, and σIW0: theoretical standard deviation of uncorrected differential intensity.