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Maintaining isobaric and isothermal conditions, we performed the relaxation up to 1.5 ns with a time step of 0.5 fs.
Hernandez-Pajares et al. (2009) showed receiver DCB values ranging from −20 to +15 ns with a variability up to a few nanoseconds.
The dc pulse field, Hdc, was applied in the negative z-direction and had a pulse width of 10 ns with a rise/fall time of 1 ns.
The standard deviation in the 4 receiver bias is from 0.370 ns to 0.855 ns, with a mean of 0.5 ns.
Hardware level simulations show a clock synchronization precision of 2 ns with a 2 GHz bandwidth signal, and an ASIC demonstrator shows 374 ps synchronization precision and 677 ps of standard deviation with the same bandwidth.
The laser pulse duration (t p ) in our case was of 57.5 ns, with a spot diameter (d), 20 μm at a frequency (f) of 100 kHz, and an average power (P) of 12 W.
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A node N with A(N)= v v is created each time c1 v, v) is chosen.
Let {u n } be a subsequence of {x n } with A({u n }) = {u} and A({x n }) = {x}.
The first cluster extends from 0 2 ns (with an average RMSD of 2.5 °A while the second cluster extends from 2.25 3.25 ns (average RMSD of ≈5.0°A).
rMD calculations were performed at constant pressure for 1 ns with an integrator time of 1 fs.
My only mode of communication was to draw the letters P-A-I-N with a finger on my palm.
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