For the sample that was treated for 17 min, the PM effect is almost the same for both orientations of the excitation polarization relative to the sample, and the ρ values at the PL maximum are equal to 0.20 (c) and 0.16 (d), for parallel and perpendicular orientation of the excitation polarization and SiOx nanocolumns projection, respectively.
Since sinusoids are leaky to protein, the liver hydrostatic tissue pressure (PL) is nearly equal to the "average" sinusoidal pressure (PS, eq. (7)).
For sets up to size 4, we can check that the COG set forms a connected subgraph by requiring that the sum of pairwise distances between COGs be smaller than or equal to max PL (line 15), the sum of distances for a linear s-node path (for s≥5, this heuristic may yield some unconnected subgraphs).
At the energy of PL maximum, the ρ values are equal to 0.22 (b) and 0.03 (a).
Using formula (1)–(4) and the same values of the optical dielectric constants, it was determined that, near PL maximum, the ρ value is equal to 0.18 if the elongated ellipsoids have a/c ≈ 0.4.
Ten of the fifteen clades that were examined in the two PL analyses have a PP value equal to or higher than 0.95 in our 28S + COI Bayesian phylogeny, and thirteen of them higher than 0.8.
For α = 0, it is clearly seen that G ↑ P is always equal to G ↓ P in the P arrangement (PL = PR = 0. 4), and the magnitudes of two peaks are equal.
From five repeated experiments of SNR10 (SNR4 data), the TPR, TNR and mFPR of GASA with AIC/no PL and GASA with BIC/PL are the same (quite close), and they are both equal to 79%, 99 % and 5 (66%66%7% and 197), respectively; while the performances of TSNI for SNR10 and SNR4 are both equal to 50%, 89% and 50%, respectively.
To obtain a resulting motion of the advantageous clone according to a given velocity relation c(Δ W), we let the difference of the two probabilities be equal to the wave velocity; i.e., | c(Δ W)| = | pl − pr|.
