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At the detector level, the principal innovation is the use of a large area (7 m2) silicon microstrip tracker.
The training of the level j consists of two steps: (1) applying the current cascaded detector (level 1 to j-1) on to generate false-positives and create a set of negative examples S n and (2) using S p and S n to train the strong classifier sign(H j -α j ).
As a consequence, we are exploring the potential application of shimming on PET detector level (for the Hyperion-IID PET/MRI insert), meaning that the distortion profile caused by PET modules is compensated using additional magnetic materials (passive shimming) and DC coils (active shimming).
All data modes were set to log, and the forward scatter detector level was set to E-1.
Samples were imaged using a Tecnai F20 Twin-transmission electron microscope operating at 120 keV at a nominal magnification of 80,000× (1.52 Å/pixel at the detector level) using a defocus range of −0.6 to −1.3 μm.
Samples were imaged in a JEOL 2200FS FEG electron microscope operated at 200 kV with a nominal magnification of 50,000 × (2.84 Å/pixel at the detector level) using a defocus range of −0.7 to −1.5 μm.
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Detector levels were adjusted such that a nonfluorescent strain had a median fluorescence of approximately 10. Populations also were gated based on forward and side scatter of the nonfluorescent strain.
Constraints are placed on models containing quark contact interactions, extra spatial dimensions, quantum black holes, or dark matter, using the detector-level distributions.
The integrated cross section and the differential cross sections as a function of top quark pT and rapidity are measured at particle level within a fiducial region related to the detector-level requirements and at parton level.
Dotted line marks the detector background level.
Optical simulation of the detector module level is highly desired for Position Emission Tomography (PET) system design.
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