Although preceding studies based their conclusions on tasks with strictly discrete reporting alternatives (e.g., "Did the object change or not?"), in continuous-report tasks participants reproduce from memory a specific feature of an object using an analog scale (e.g., Bays, Catalao, & Husain, 2009; Wilken & Ma, 2004; Zhang & Luck, 2008).
Mass and momentum are strictly conserved at discrete level while the method allow for energy dissipation only in the case of wave breaking and provide comparable results with those of extended Boussinesq models [3, 10, 12].
It should also be noted that substance abuse is not, strictly speaking, a discrete event, but an ongoing condition.
If time is understood as a succession of discrete moments, then, strictly speaking, our experience will be one of perpetual loss: every instant, every unit of time, is a mere passing from that which has not yet been to that which will never again be, and the passing itself will not endure but simply be a boundary between future and present.
For n -order derivatives and differences, n > 1, the constants in the discrete inequalities are strictly greater than those in the continuous case, the corresponding θ ∗ = 1 - 1 / ( 2 n ).
Given the lack of quantitative information about reaction kinetics, a reasonable approach is to use Boolean models, which represent concentrations of proteins with a few discrete qualitative levels (strictly interpreted, the term "Boolean" implies variables can only take two values, but we use it in the more general sense that allows more than two discrete levels variables).
These operators arise by replacing the discrete Laplacian by a strictly increasing C1-function of the discrete Laplacian.
We first present a sufficient condition for extended strictly positive realness of 2-D discrete delayed systems.
In the present paper we consider a class of Schrödinger operators obtained as a strictly increasing C1-function of the discrete Laplacian and a δ-potential.
The next theorem states that for higher order inequalities the constants in the discrete case are always strictly greater than those in the continuous case.
Since (1 pmsin{t}) and (1 pmcos{t}) are positive except at discrete points, (31) shows that (varphi_) is strictly increasing and (varphi_) is strictly decreasing on the intervals where they are defined.
