| Sammanfattning: | We study the diffusion of tagged hard-core interacting Brownian point particles under the influence of an
external force field in one dimension. Using the Jepsen line we map this many-particle problem onto a single
particle one. We obtain general equations for the distribution and the mean-square displacement {(xT)[superscript 2]} of the tagged center particle valid for rather general external force fields and initial conditions. The case of symmetric distribution of initial conditions around the initial position of the tagged particle on x=0 and symmetric
potential fields V(x)=V(−x) yields zero drift {xT}=0 and is investigated in detail. We find {(xT)superscript 2]}=R(1−R)/2Nr[superscript 2] where 2N is the (large) number of particles in the system. R is a single particle reflection coefficient,i.e., the probability that a particle free of collisions starts on x[subscript 0]>0 and remains in x>0 while r is theprobability density of noninteracting particles on the origin. We show that this equation is related to themathematical theory of order statistics and it can be used to find {(xT)[superscript 2]} even when the motion betweencollision events is not Brownian (e.g., it might be ballistic or anomalous diffusion). As an example we derive the Percus relation for non-Gaussian diffusion. A wide range of physical behaviors emerge which are very
different than the classical single file subdiffusion {(xT)[superscript 2]}~t[superscript 1/2] found for uniformly distributed particles in an infinite space and in the absence of force fields.
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