Deep learning enhanced fluorescence fluctuations super-resolution microscopy

Fluorescence fluctuations super-resolution microscopy (FF-SRM) is a powerful tool in imaging and monitoring of biological subcellular structures and dynamics in cells. A variety of image reconstruction algorithms have been developed for FF-SRM. In order to obtain high spatiotemporal resolution, a U-Net-based deep learning method for super-resolution imaging of fluorescence fluctuations was developed. With just 20 frames, super-resolution images reconstructed using U-Net model could be comparable to those reconstructed using VeSRRF algorithm with several hundred frames, demonstrating its capability of advancing imaging capabilities.

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Publication Details

Published
2024-10-08
DOI
https://doi.org/10.1117/12.3039254
Citations
1
Primary Topic
Advanced Fluorescence Microscopy Techniques
Type
article
Field-Weighted Citation Impact
0.66
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article

Deep learning enhanced fluorescence fluctuations super-resolution microscopy

Yanru Li, Lin Wang, Lixin Liu
1 citations
Advanced Fluorescence Microscopy Techniques
0.66
article

Deep learning enhanced fluorescence fluctuations super-resolution microscopy

Yanru Li, Lin Wang, Lixin Liu
article en
1 citations

Abstract

Fluorescence fluctuations super-resolution microscopy (FF-SRM) is a powerful tool in imaging and monitoring of biological subcellular structures and dynamics in cells. A variety of image reconstruction algorithms have been developed for FF-SRM. In order to obtain high spatiotemporal resolution, a U-Net-based deep learning method for super-resolution imaging of fluorescence fluctuations was developed. With just 20 frames, super-resolution images reconstructed using U-Net model could be comparable to those reconstructed using VeSRRF algorithm with several hundred frames, demonstrating its capability of advancing imaging capabilities.

Rutherford Appleton Laboratory (GB), Xidian University (CN), Shenzhen University (CN)
Openalex Percentile: Top 19%
Advanced Fluorescence Microscopy Techniques
0.66
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