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At the detector level, the principal innovation is the use of a large area (7 m2) silicon microstrip tracker.
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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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.
The decision whether a pulse occurs in the current chip is made according to the threshold level at the detector.
For all other experiments thereafter, the detector gain level was kept constant at all excitation wavelengths and for both WI and MI.
Dotted line marks the detector background level.
Because the detectors use Superconducting Quantum Interference Devices (SQUIDs), the field at the detector package must remain at or below the 10−7 T level while the detectors are operating.
At the detector's heart is 370kg (815lb) of liquid xenon.
With the simulated power level distribution at the detectors mounted on a Luneburg lens, both Cramér-Rao bound (CRB) and the root mean square error (RMS) based on the Correlation Algorithm (CA) for the direction of arrival (DoA) estimation have been derived and calculated.
This detector features an innovative readout integrated circuit, the second version of the Fermilab Silicon Strip Readout chip (FSSR2), which, being completely data-driven, allows for the direct use of the detector information at the lowest level of the trigger.
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