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First, the system can ensure access to high-quality images from a stable light source environment by adding the hoods and LED auxiliary light source in the image acquisition equipment.
In contrast, to determine the coordinates of the wave source in the image plane we have to deal with spatial intensity distributions which are more sensitive to noise and tissue heterogeneity.
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The number of counts in a region-of-interest (ROI) around the source in the images was determined and plotted versus the depth.
The diffuse emission is hot gas in the cluster and other point-like sources in the image are nearly all unrelated to the galaxy cluster.
It is important to also note that images of the family depend upon the specific source in which the image is found and the type of audience that the source aims to reach.
To check that, the team reverted to a much more complex piece of hardware: the ILL's world-beating neutron source, seen in the image above.
This binned data is represented in Fig. 6(a) which shows the intensity decay from 0.7 to 2 cm for an exposure time of 1 ms. Here it is also observed that the sensor was not saturated at shorter distances from the source available in the image and that at 2 cm the intensity was still decaying as expected from the diffusion theory.
To the south of the source in the deconvolved image, there appears to be an unresolved blob, which in all likelihood is not physically real.
Note that we can also select a source in the DS9 image display to have it simultaneously highlighted in a TOPCAT table or plot (as well as in the CSCview results table).
As a result, the spatial resolutions of a Na-22 point source in the PET image were lower than 1.6 mm in whole the FOV due to the DOI capability.
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