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ACQUISITION AND DISPLAY OF ULTRA HIGH-RESOLUTION BACKSCATTERED ELECTRON IMAGES OF METEORITE SECTIONS R. C. Ogliore, Washington University in St. Louis ([email protected]) Why Ultra-Res BSE? Ultra-Res BSE: Backscattered electron imaging at ~50 nm per pixel over an entire 1-inch round thin/thick meteorite section “Virtual Microscope” allows for remote characterization of sample mineralogy/petrology Facilitates searching for small rare phases (e.g., cosmic symplectite, carbonaceous microclasts) Minimizes electron beam exposure for beam-sensitive samples Especially useful for rare/precious/fragile samples: CI chondrites, returned samples from Hayabusa2 and OSIRIS-REx missions Challenges Acquisition: Sample topography is larger than the depth-of-field at high magnifications — focus changes across sample Balance: Brightness/contrast variations due to sample-detector geometry and changing emission current Robustness: Deal with outliers (bad stage move, no features for alignment) Stitching: Extreme large final image size (up to 250 gigapixels) makes mosaic assembly dicult due to memory requirements Display: Large final image makes display challenging Solutions to Challenges Acquisition: First acquire “focus map” over entire sample and calculate objective-lens working distance (by surface fitting or 2D interpolation) for a matrix of high-resolution acquisitions of ~10,000 individual BSE images. Balance: Use overlap in stitching and recorded emission current to calculate brightness changes across individual BSE images. Solutions to Challenges (continued) Robustness: Calculate positions/rotations of each image from matched features in Matlab using an ane geometric transform, then remove outliers and interpolate. Each image one 3×3 ane matrix. Stitching: Use pyvips (pixel streaming) and ane matrices calculated from Matlab to stitch final mosaic. Display: Create deepzoom image tiles in pyvips and display in OpenSeaDragon in web browser, with scale bar and other features for easy cataloging of small features. Conclusions Tescan Mira3 FEG-SEM with ImageSnapper plugin was used for this work, but can be adapted to other SEMs All code to acquire, stitch, and display ultra-res BSE images is available on github: https://github.com/ ogliore/DeepZoomSEM Example images: https://presolar.physics.wustl.edu/ meteorite-deep-zoom/ Future improvements: 16-bit image display with real- time image adjustments, false-color options, processing speed improvements.
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ACQUISITION AND DISPLAY OF ULTRA HIGH-RESOLUTION ... · ACQUISITION AND DISPLAY OF ULTRA HIGH-RESOLUTION BACKSCATTERED ELECTRON IMAGES OF METEORITE SECTIONS R. C. Ogliore, Washington

Sep 23, 2020

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Page 1: ACQUISITION AND DISPLAY OF ULTRA HIGH-RESOLUTION ... · ACQUISITION AND DISPLAY OF ULTRA HIGH-RESOLUTION BACKSCATTERED ELECTRON IMAGES OF METEORITE SECTIONS R. C. Ogliore, Washington

ACQUISITION AND DISPLAY OF ULTRA HIGH-RESOLUTION BACKSCATTERED ELECTRON IMAGES OF METEORITE SECTIONS

R. C. Ogliore, Washington University in St. Louis ([email protected])

Why Ultra-Res BSE? • Ultra-Res BSE: Backscattered electron imaging at ~50 nm per pixel over an entire 1-inch round thin/thick meteorite section • “Virtual Microscope” allows for remote characterization of sample mineralogy/petrology • Facilitates searching for small rare phases (e.g., cosmic symplectite, carbonaceous microclasts) • Minimizes electron beam exposure for beam-sensitive samples • Especially useful for rare/precious/fragile samples: CI chondrites, returned samples from Hayabusa2 and OSIRIS-REx missions

Challenges • Acquisition: Sample topography is larger than the depth-of-field at high magnifications — focus changes across sample • Balance: Brightness/contrast variations due to sample-detector geometry and changing emission current • Robustness: Deal with outliers (bad stage move, no features for alignment) • Stitching: Extreme large final image size (up to 250 gigapixels) makes mosaic assembly difficult due to memory requirements • Display: Large final image makes display challenging

Solutions to Challenges • Acquisition: First acquire “focus map” over entire sample and calculate objective-lens working distance (by surface fitting or 2D interpolation) for a matrix of high-resolution acquisitions of ~10,000 individual BSE images.

• Balance: Use overlap in stitching and recorded emission current to calculate brightness changes across individual BSE images.

Solutions to Challenges (continued) • Robustness: Calculate positions/rotations of each image from matched features in Matlab using an affine geometric transform, then remove outliers and interpolate. Each image → one 3×3 affine matrix. • Stitching: Use pyvips (pixel streaming) and affine matrices calculated from Matlab to stitch final mosaic.• Display: Create deepzoom image tiles in pyvips and display in OpenSeaDragon in web browser, with scale bar and other features for easy cataloging of small features.

Conclusions • Tescan Mira3 FEG-SEM with ImageSnapper plugin was used for this work, but can be adapted to other SEMs • All code to acquire, stitch, and display ultra-res BSE images is available on github: https://github.com/ogliore/DeepZoomSEM • Example images: https://presolar.physics.wustl.edu/meteorite-deep-zoom/ • Future improvements: 16-bit image display with real-time image adjustments, false-color options, processing speed improvements.