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Based on this equation, the detector current response R λ of a single UAN is over 2.7×106, which is much bigger than many nanostructures.
The following chromatographic conditions were used: carrier gas, He; injector T, 120°C; oven T, 70°C; detector T, 120°C; detector type, thermal conductivity; detector current, 120 mA.
The true brightness 〈 ɛ〉 and the true number of particles n are thus dependent on the calibration of the instrument when using analog detectors (30), because one needs to consider the internal variance of the detector current, which is a linear function of the detector current and the readout term.
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The power reduction escalates further for higher detector currents and large format Focal Plane Arrays (FPA).
The detector currents were monitored during irradiation, which allows the predictions of bulk radiation damage parameterizations to be tested.
The measurement system is designed to have a Si n+ p p+ detector and current amplifier.
The conventional decision-directed methods will fail in this situation because all of them feed the previous estimates to the MMSE detector for current detection.
To prove the feasibility of the idea we first tested the performance of a special non-windowed SiPM by Hamamatsu (MPPC) as electron detector and current amplifier.
The detector dark current density is 5.3 ± 0.2 μatcm2 at −1 V bias, and with a peak external quantum efficiency of 12.6 ± 0.3% at a wavelength of 640 nm.
Operating the device at −20°C we have obtained a map of detector dark current, which is typically in the range 0.4 pA to 0.8 pA/pixel.
The detector dark current as a function of bias voltage, presented in Figure 2, was measured with a cold shield to eliminate background radiation for various temperatures from 90 to 120 K. Also shown in Figure 2 is the photocurrent measured at 80 K with the device illuminated from the 300-K background radiation (field of view = 53°).
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