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In matching the WS parameters K, p, n to the target system, we know n, can measure 〈k〉 (giving K = 〈k〉/2), but estimating p has, hitherto, remained problematic.
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Figure 5 Doppler broadening spectroscopy of S - W parameters vs. positron incident energy.
The S and W parameters were calculated to characterize Doppler broadening.
W parameters are higher and S parameters are lower when annihilation of the core electrons of atoms occurs.
In sum, the values of, and W parameters must be jointly decided upon, making trade-offs between throughput and delay.
The membership functions form a Ruspini partition with u, v, and w parameters as can be seen in Fig. 9.
The S vs. W diagrams of monolithic materials present clusters of points because all S or W parameters are almost the same [14].
The formation of vacancy-like defects surrounded by tiny Cu precipitates induced the increment of the S and W parameters after irradiation.
The shape of 511-keV annihilation line obtained for studied samples was analyzed by determining so-called S and W parameters [27].
(a) S and (b) W parameters vs. positron incident energy for samples annealed at different temperatures for 10 min. (c) S-W plot for samples annealed at different temperatures for 10 min. The S and W parameters of the same incident energy were plotted in one graph, as shown in Figure 5c.
Baseline records for slow wave sleep (SWS) and wake (W) parameters were unchanged, whereas paradoxical sleep (PS) episode numbers were decreased and PS latency increased after lights off in hSODwt/+ mice versus controls.
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