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Image Search Results
Journal: Biomedical Optics Express
Article Title: Rapid multi-plane phase-contrast microscopy reveals torsional dynamics in flagellar motion
doi: 10.1364/BOE.419099
Figure Lengend Snippet: Inter-plane distance and brightness calibration. (a) Example of the eight images of scattering microspheres recorded by the multi-plane wide-field microscope. In this example, microspheres are in focus in nominal plane #4 (b) Normalized average intensity in each image plane as a function of axial scan position (for axial scan steps of 100 nm). Crosses (for camera 1) and open circles (for camera 2) represent measured data, solid lines are Gaussian fits. (c) Linear fit of positions of intensity maxima from panel (b). The fit yields an average inter-plane distance of 430 nm (for oil immersion). (d) Relative shift of focal plane position in water (blue line) with respect to oil (red line). Open circles are the result of a wave-optical calculation of imaging in water, the blue solid line is a linear fit to this result. It shows that close to the glass interface, we still find a linear relationship between focal plane position and the objective’s axial position, but inter-plane distance in water is by a factor of 0.78 smaller than in oil.
Article Snippet: For noise reduction, a
Techniques: Microscopy, Imaging
Journal: Scientific Reports
Article Title: Prior Experience Alters the Appearance of Blurry Object Borders
doi: 10.1038/s41598-020-62728-y
Figure Lengend Snippet: Blur levels for Lamp stimulus. Depiction of Test blur levels used for all experiments applied to the familiar stimulus used in Experiments 1–3, the silhouette of a lamp. The blur level refers to the standard deviation (in pixels) of the Gaussian distribution that gave its shape to the smoothing kernel used to blur the stimuli (see Methods for more explication). The blur level of the Standard stimulus was always 7 pixels.
Article Snippet: Before each trial, each stimulus was blurred to its assigned blur level using
Techniques: Standard Deviation
Journal: Journal of Cell Science
Article Title: CTRL – a label-free artificial intelligence method for dynamic measurement of single-cell volume
doi: 10.1242/jcs.245050
Figure Lengend Snippet: DIC image and cell topography fluorescence image pre-processing. (A) DIC image pre-processing. For each DIC image, we first cropped the image to obtain single cells with the least amount of background (A1). We then acquired a background mask by taking a 10 pixel band closest to the edge (A2). A polynomial fitting using the function ‘poly22’ in MATLAB was applied to perform an intensity fitting to the background mask (A3). The image in A3 is subtracted from the image in A1 to obtain a background-corrected image A4. The purpose of this background correction is to reduce the potential local intensity heterogeneity within one DIC image. After background correction, we acquired a new background mask A5 based on the background-corrected image with the same procedure and created a new artificial background ‘canvas’ for cell padding A6. The ‘canvas’ of size 512×512 was created by generating a Gaussian distribution with the same mean and standard deviation as the background mask acquired in A5. The background-corrected cell in A4 was then put into the middle of A6 to finalize the background padding (A7). Finally, we normalized the image to the data type of uint8 (8-bit) with integer values between 0 and 255 (A8). (B) Cell topography fluorescence image pre-processing. A background intensity polynomial fitting (B2) was first applied to the original fluorescence image (B1) using the same procedure as described in the ‘DIC image pre-processing’ section. The estimated height of the cell at each pixel hpixel is directly proportional to the loss of intensity at the pixel. For instance, if the pixel intensity is 0, then the height at the pixel is the height of the microchamber; if the intensity is the maximum intensity, then the height of the cell at the pixel is 0:hpixel = (1-Ipixel/Ichannel) × hchannel. The relative pixel intensity (B3) Ipixel/Ichannel was then obtained by dividing B1 by B2 for each pixel. The image B3 was then subtracted by 1 and multiplied by the value of microchamber height hchannel to reflect the height of the cell at each pixel (in μm units) as shown in B4. (Note due to optical effects, the intensity only estimates the height. However, the integrated intensity over the image reports the true volume image.) An artificial background ‘canvas’ (B5) was created for padding using the same procedure as described in the ‘DIC image pre-processing’ section. The cell image was put into the center of the ‘canvas’ as shown in B6, and a binary-valued cell mask was created by thresholding over the value of 0.05 and dilating approximately 30 pixels outwards (away from the cell) using MATLAB function ‘imdilate’ (B7). The binary mask with the value 0 in the background and the value 1 inside the dilated region was then multiplied to the image in B6 to obtain a cleaned cell image B8 with the intensity of all pixels in the artificial background cleared to zero. Finally, a Gaussian filter using MATLAB function ‘imgaussfilt’ with a 2D Gaussian smoothing kernel with standard deviation value of 3 was applied to the image to obtain a smoothed cell topography (B9). This step does not change the integrated cell volume.
Article Snippet: Finally, a Gaussian filter using
Techniques: Fluorescence, Standard Deviation
Journal: Journal of Cell Science
Article Title: CTRL – a label-free artificial intelligence method for dynamic measurement of single-cell volume
doi: 10.1242/jcs.245050
Figure Lengend Snippet: DIC image and cell topography fluorescence image pre-processing. (A) DIC image pre-processing. For each DIC image, we first cropped the image to obtain single cells with the least amount of background (A1). We then acquired a background mask by taking a 10 pixel band closest to the edge (A2). A polynomial fitting using the function ‘poly22’ in MATLAB was applied to perform an intensity fitting to the background mask (A3). The image in A3 is subtracted from the image in A1 to obtain a background-corrected image A4. The purpose of this background correction is to reduce the potential local intensity heterogeneity within one DIC image. After background correction, we acquired a new background mask A5 based on the background-corrected image with the same procedure and created a new artificial background ‘canvas’ for cell padding A6. The ‘canvas’ of size 512×512 was created by generating a Gaussian distribution with the same mean and standard deviation as the background mask acquired in A5. The background-corrected cell in A4 was then put into the middle of A6 to finalize the background padding (A7). Finally, we normalized the image to the data type of uint8 (8-bit) with integer values between 0 and 255 (A8). (B) Cell topography fluorescence image pre-processing. A background intensity polynomial fitting (B2) was first applied to the original fluorescence image (B1) using the same procedure as described in the ‘DIC image pre-processing’ section. The estimated height of the cell at each pixel hpixel is directly proportional to the loss of intensity at the pixel. For instance, if the pixel intensity is 0, then the height at the pixel is the height of the microchamber; if the intensity is the maximum intensity, then the height of the cell at the pixel is 0:hpixel = (1-Ipixel/Ichannel) × hchannel. The relative pixel intensity (B3) Ipixel/Ichannel was then obtained by dividing B1 by B2 for each pixel. The image B3 was then subtracted by 1 and multiplied by the value of microchamber height hchannel to reflect the height of the cell at each pixel (in μm units) as shown in B4. (Note due to optical effects, the intensity only estimates the height. However, the integrated intensity over the image reports the true volume image.) An artificial background ‘canvas’ (B5) was created for padding using the same procedure as described in the ‘DIC image pre-processing’ section. The cell image was put into the center of the ‘canvas’ as shown in B6, and a binary-valued cell mask was created by thresholding over the value of 0.05 and dilating approximately 30 pixels outwards (away from the cell) using MATLAB function ‘imdilate’ (B7). The binary mask with the value 0 in the background and the value 1 inside the dilated region was then multiplied to the image in B6 to obtain a cleaned cell image B8 with the intensity of all pixels in the artificial background cleared to zero. Finally, a Gaussian filter using MATLAB function ‘imgaussfilt’ with a 2D Gaussian smoothing kernel with standard deviation value of 3 was applied to the image to obtain a smoothed cell topography (B9). This step does not change the integrated cell volume.
Article Snippet: Finally, a
Techniques: Fluorescence, Standard Deviation