Spectrometer Noise Reduction via Segmented Exposure Averaging

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Solution Overview

Problem

Optical spectrometers face challenges in minimizing nonrandom noise sources, which cannot be addressed by lengthening single exposures, as these types of noise do not average out over time and often increase with longer exposures, limiting the signal-to-noise ratio (SNR).

Innovation Solution

An automated system and method that calculates a total observation time by averaging multiple exposures of predetermined time, based on the noise characteristics of the spectrometer system, to minimize nonrandom noise sources such as flicker or 1/f noise, independent of sample signal intensity, allowing for improved SNR without user input.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If single exposure time is lengthened to minimize random noise (Johnson-Nyquist and shot noise), then signal-to-noise ratio improves, but nonrandom noise (flicker or 1/f noise) increases and cannot be minimized

Engineering Contradiction:
Improvesignal-to-noise ratioVSAvoidnonrandom noise
Core Design Contradiction:
Measurement precisionVSObject-affected harmful factors

Solution Approach 1:

The patent divides a single long exposure into multiple shorter exposures. Each short exposure minimizes nonrandom noise accumulation, while the results are combined through averaging to achieve the desired signal-to-noise ratio. This segmentation approach directly resolves the contradiction by preventing nonrandom noise from dominating while still achieving sufficient integration time.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent employs periodic repeated exposures rather than a single continuous exposure. Multiple exposures are performed in sequence and averaged together, creating a periodic measurement process that minimizes nonrandom noise in each cycle while achieving the required observation time through repeated cycles.

Inventive Principle:
Principle #19Periodic action

2Measurement precision

If multiple exposures are summed or averaged to achieve longer observation time, then random noise is minimized, but readout noise is introduced and overall noise increases

Engineering Contradiction:
Improvesignal-to-noise ratioVSAvoidreadout noise
Core Design Contradiction:
Measurement precisionVSObject-generated harmful factors

Solution Approach 1:

The patent changes the exposure time parameter to be shorter than the detector saturation limit. By using short exposures that do not saturate the detector, the method avoids introducing excessive readout noise while still achieving the required signal-to-noise ratio through multiple exposures. This parameter optimization resolves the contradiction by finding the optimal exposure duration.

Inventive Principle:
Principle #35Parameter changes

3Illumination intensity

If maximum exposure time is used to saturate the detector, then signal intensity is maximized, but nonrandom noise cannot be minimized and measurement precision is limited

Engineering Contradiction:
Improvesignal intensityVSAvoidsignal-to-noise ratio
Core Design Contradiction:
Illumination intensityVSMeasurement precision

Solution Approach 1:

The patent uses partial action by employing exposures that are shorter than the maximum saturation time. Instead of maximizing signal intensity through saturation, the method uses controlled short exposures that provide sufficient signal while minimizing nonrandom noise, achieving a better overall signal-to-noise ratio through multiple such exposures.

Inventive Principle:
Principle #16Partial or excessive action

Data Source

PatentUS11313720B2System and method to minimize nonrandom fixed pattern noise in spectrometers
Publication Date: 2022.04.26 RIGAKU RAMAN TECH INC
  • US11313720B2 patent drawing
  • US11313720B2 patent drawing
  • US11313720B2 patent drawing

AI summary

This invention relates to a system and method to improve the signal to noise ratio (SNR) of optical spectrometers that are limited by nonrandom or fixed pattern noise. A signal from a sample is collected using a short test exposure, a total observation time to maximize SNR is calculated, and the total observation time is achieved by averaging multiple exposures whose time is selected based on the time dependent noise structure of the detector. Moreover, with a priori knowledge of the time dependent noise structure of the spectrometer, this method is easily automatable and can maximize SNR for a spectrum of an unknown compound without any user input.