Abstract

Fringe patterns encode the information about the result of a measurement performed via widely used optical full-field testing methods, e.g., interferometry, digital holographic microscopy, moiré techniques, structured illumination etc. Affected by the optical setup, changing environment and the sample itself fringe patterns are often corrupted with substantial noise, strong and uneven background illumination and exhibit low contrast. Fringe pattern enhancement, i.e., noise minimization and background term removal, at the pre-processing stage prior to the phase map calculation (for the measurement result decoding) is therefore essential to minimize the jeopardizing effect the mentioned error sources have on the optical measurement outcome. In this contribution we propose an automatic, robust and highly effective fringe pattern enhancement method based on the novel period-guided bidimensional empirical mode decomposition algorithm (PG-BEMD). The spatial distribution of the fringe period is estimated using the novel windowed approach and then serves as an indicator for the truly adaptive decomposition with the filter size locally adjusted to the fringe pattern density. In this way the fringe term is successfully extracted in a single (first) decomposition component alleviating the cumbersome mode mixing phenomenon and greatly simplifying the automatic signal reconstruction. Hence, the fringe term is dissected without the need for modes selection nor summation. The noise removal robustness is ensured employing the block matching 3D filtering of the fringe pattern prior to its decomposition. Performance validation against previously reported modified empirical mode decomposition techniques is provided using numerical simulations and experimental data verifying the versatility and effectiveness of the proposed approach.

Highlights

  • Fringe analysis is a central aspect of many contemporary full-field optical measurement techniques, i.e., interferometry, fringe projection and quantitative phase imaging, crucial in nowadays technical and biomedical non-contact investigations

  • It is highly desirable to avoid the mode mixing, e.g., using the sinusoid assisted decomposition [57] or employing the automatic selective reconstruction scheme [48], and/or concentrate the fringe part in a single mode, e.g., modifying the envelope construction part [58]. In this contribution we present a novel technique named the period-guided bidimensional empirical mode decomposition (PG-bidimensional EMD (BEMD)), able to extract a complete fringe component condensed in the first mode using the local fringe density map guidance

  • In the presented period-guided bidimensional empirical mode decomposition algorithm (PG-BEMD) approach we propose to use the sliding-window filtering and spatially vary the width of the squared window adjusting it to the local fringe pattern density

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Summary

Introduction

Fringe analysis is a central aspect of many contemporary full-field optical measurement techniques, i.e., interferometry, fringe projection and quantitative phase imaging, crucial in nowadays technical and biomedical non-contact investigations. The practical impact of the BEMD was severely limited by the calculation time – the spline interpolation on the irregular grid is the most expensive part of the algorithm It was even more of an issue in 2D ensemble EMD [40,41], technique for the noise-assisted data analysis with increased efficiency of the signal component separation. It is worth showcasing that variational image decomposition techniques, recently flourishing in the fringe analysis [59,60], operate on a notion of sparsely extracting single fringe component They stay out of the scope of this study due to significantly distinctive modus operandi of the decomposition based on the total variation approach and the iterative projection algorithm

Working principle of the PG-BEMD and selected reference methods
PG-BEMD: boundary aware fringe pattern envelope estimation
Numerical evaluation using synthetic fringe patterns
The BM3D-based solution to the noise transferring problem
Experimental validation
Closing remarks
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