ABSTRACT: A harmonic function of the Brownian path is a local martingale. Is the converse true? We show that the class of local martingale functions of Brownian motion is co-extensive with the class of finely harmonic functions, and then use a results of Fuglede and Gardiner to answer this question in the negative, in dimensions bigger than 2.
With the demand from modeling systems level cellular biochemistry as a reaction network, different applied mathematical approaches are now being pursued. I will discuss three approaches based on (1) systems of ODE with nonlinearity, (1) stochastic processes with irreversibility, and (3) constraint-based optimization suggesting an oriented matroid. A unifying theme of these approaches is the nonequilibrium thermodynamics of living (open) systems.
In the glucose-insulin regulatory system, insulin secretion oscillates with a period of 50-150 minutes. Over the past decade, several mathematical models have been proposed to model these ultradian oscillations as well as the metabolic system producing them. However these existing models yield profiles deviant from a normal physiological range. We introduce a DDE (delay differential equation) model with two discrete delays for better understanding and more accurately modeling the glucose-insulin dynamics and the insulin secretory oscillations. With the same set of experimental data used to test other existing models, the simulation profiles obtained from this two time delay model fall within a normal physiological range.
We consider the edge Hall conductance and show it is invariant under perturbations located in a strip along the edge. This enables us to prove for the edge conductances a general sum rule relating currents due to the presence of two different media located respectively on the left and on the right half plane. As a particular interesting case we put forward a general quantization formula for the difference of edge Hall conductances in semi-infinite samples with and without a confining wall. Applications to disordered Hall systems with and without a confining potential are discussed.
We consider the edge Hall conductance and show it is invariant under perturbations located in a strip along the edge. This enables us to prove for the edge conductances a general sum rule relating currents due to the presence of two different media located respectively on the left and on the
right half plane. As a particular interesting case we put forward a general quantization formula for the difference of edge Hall conductances in semi-infinite samples with and without a confining wall. Applications to disordered Hall systems with and without a confining potential are discussed.