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This time span is directly proportional to the EPSC width at half amplitude, which is almost entirely determined by the decay time constant as demonstrated by the fact that STP vs. decay time and STP vs. half width are almost identical functions (Figure 2C, D).
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The corresponding half width is 364.4 kW.
For low-angle GBs, an apparent transition of PFZ half width is observed at a misorientation of 11°.
AP half width was measured at half-maximal amplitude.
Mean amplitudes of mIPSCs amounted to 84 + 16 pA, mean rise times were 1.4 + 0.2 ms and mean widths of events at the level of half of the amplitude (half width) was 13.8 + 1.7 ms (n = 6; Figure 5A).
The half width was defined as the full-width at half maximum of PCr, respectively, P i. SNR was defined as the ratio between the PCr- and P i -peak amplitude and the peak-to-peak spectral noise, in the range of +10 to +20 ppm.
The half widths were measured as the time between maximal and minimal peaks for each response half cycle.
The coherent structures of the flow developing around a surface-mounted cubic obstacle placed in turbulent channel flow (Re=40.000 based on bulk velocity and channel half-width) are investigated.
As observed for the 2Cys47 unfolded peak, the apparent spFRET peak efficiency for the 2Cys313 unfolded peak decreases with increasing GdmCl concentrations, and the half-widths are wider than those predicted from shot noise.
Instrumental error was estimated using the etalon, and corrections for the reflex half-width were calculated.
In addition, the equatorward half-width was correlated with the trough minimum position; the correlation between the two was 0.55.
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