This trend should generate a reduced variance in length at maturity (or length at spawning) – this is indeed what we observe also when looking at the observed variation for length at spawning over time (Fig. 6).
An alternative interpretation may be that the enhanced phosphorylation of CTLA4 we observe also increases the rate of internalization, such that there is no observable change in surface expression.
We observe also that the gain in achievable rates is high for high values of δSNR.
We can observe also that the theoretical PLR performances as given by (17) agree with the simulation results.
We observe also on Fig. 19 a steeper variation of p θ (t) at t=5.86 s.
We observe also that the performance is moderate when the channel conditions change frequently (the coherence time is small).
We observe also in this table that the local Nusselt number decreases as the fluid variable viscosity parameter increases.
We observe also the differences in the thermal stability of devices – characteristic temperature is lower for lasers with 3% Al in EBL.
At present time it is possible to observe also an increasing interest in research field of the UHPC in many countries.
From Tables 3, 4 and 5, we observe also that the λ 2-continuation causes most failures in the non-planar case.
Let us observe also that, if A is α-inverse strongly monotone, the mappings P C ( I − λ A ) are nonexpansive for all λ ∈ ( 0, 2 α ] since they are compositions of nonexpansive mappings (see [[37], pp.419]).
