Exact(13)
The S1 state typically exists for 1 100 nanoseconds (ns; 1 ns is 10−9 second), but if photochemistry occurs, it can exist for less than 100 fs.
Table 4 Computational complexity of the proposed algorithm Feature Number of operations Complex multiplication Complex addition Comparison K 1 0 Ns – 1 2Ns + 1 K 2 0 Ns – 1 3Ns + 1 K 3 0 Ns – 1 2Ns + 1 K 4 0 Ns – 1 4Ns + 1 K max Ns/2log(Ns) + Ns + 1 Ns log(Ns) N s Γ1 Ns/2log(Ns) + Ns + 1 Ns log(Ns) N s Γ2 Ns/2log(Ns) + 2Ns + 1 Ns log(Ns) N s Γ4 Ns/2log(Ns) + 4Ns + 1 Ns log(Ns) N s.
The nonstructural (NS) 1 protein of A/common buzzard/Bulgaria/38WB/2010 is encoded by 230 aa.
Equations for white-tailed ptarmigan are the same except ASY females were assumed to have a probability of re-nesting a second time [ 13]: (6) F SY = C 1 SY ns 1 + 1 − ns 1 r 1 SY C 2 ns 2 S JUV 0.5 (7) F ASY = C 1 ASY ns 1 + 1 − ns 1 r 1 ASY C 2 ns 2 + 1 − ns 1 1 − ns 2 r 1 ASY r 2 ASY C 2 ns 2 S JUV 0.5 where r1ASY and r2ASY are the ASY re-nest probabilities for 2nd and 3rd attempts.
2. Shear-thinning Alakali et al. (2009) Cissus populnea NS 1. < Apparent Visc.
Cassava starch NS 1. < Apparent viscosity with > shear rate 2. Shear-thinning Che et al. (2008) Dilute cassava starch NS 1. Shear-thinning, 2. Change from Newtonian to Non-Newtonian @ > 0.4% Conc.
Similar(47)
The pulses for RESET and SET operations are 0.5 mA (10 ns)−1 and 0.2 mA (100 ns)−1, respectively.
Again, the parameter combination (Ns)−1 has a simple interpretation as the variance of the stochastic effects accumulated over time s−1.
The ACF complexity around Na(Ns- 1)(L + 1 3 floating-point operations.
Hence, the TR complexity around Na(Ns- 1)(p + 1 3 floating-point operations [13].
whose rate constant kDC is (3.8 ns)− 1.
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