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We first note that the fixed point of the dynamics remains unchanged as (w_{E} + w_{I}) increases from ({0.8 rightandow13.8}), an_{(n_{E} = n_{I}).
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The space of solutions to (9) is the convex polyhedral cone of networks having each clique as a strict local minimum of the energy function, and thus a fixed-point of the dynamics.
Thus, resulting fixed-points (of the dynamics) end up being graphs such as cliques and stars.
From a mathematical point of view, the dynamics of the model is (numerically) solving the differential equations of LP1 to LP17 by assuming that at time t = 0, WS s) and WS(c) holds value 1 as state level.
But also suppose that at this point of time the dynamics of the measuring apparatus reverts to the orthodox linear Schrödinger form.
From the control point of view, the dynamics of nonholonomic systems can be divided in two parts: external and internal dynamics.
From a biological and therapeutic point of view, the dynamics of AR status during tumor progression is an important consideration.
From a system study point of view the dynamics are divided into two kinds of simulations, i.e. electromagnetic transient and electromechanical transient simulations.
In this connection, it is interesting to note the following [2]: Every Nash equilibrium is a fixed point of the replicator dynamics and the game-dynamical equation.
However, it becomes a saddle point of the full dynamics in the (q, p) plane, reflecting the fact that it is metastable when fluctuations are taken into account.
RDCs of the inner iduronic acid were calculated for every point of the molecular dynamics trajectory.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com