Dover, Y. (2004).
A short account of a connection of power laws to the information entropy.
Physica A: Statistical Mechanics and its Applications ,
334 (3-4).
AbstractWe use the formalism of "maximum principle of Shannon's entropy" to derive the general power law distribution function, using what seems to be a reasonable physical assumption, namely, the demand of a constant mean "internal order" (Boltzmann entropy) of a complex, self-interacting, self-organized system. Since the Shannon entropy is equivalent to the Boltzmann's entropy under equilibrium, non-interacting conditions, we interpret this result as the complex system making use of its intra-interactions and its non-equilibrium in order to keep the equilibrium Boltzmann's entropy constant on the average, thus enabling it an advantage at surviving over less ordered systems, i.e., hinting towards an "Evolution of Structure". We then demonstrate the formalism using a toy model to explain the power laws observed in Cities' populations and show how Zipf's law comes out as a natural special point of the model. We also suggest further directions of theory. © 2003 Elsevier B.V. All rights reserved.
Balberg, I., Dover, Y., Naides, R., Conde, J. P., & Chu, V. (2004).
State distribution in hydrogenated microcrystalline silicon.
Physical Review B - Condensed Matter and Materials Physics ,
69 (3).
AbstractWe have been able to determine the density of states map in the band gap of a semiconductor by the measurement of the phototransport properties of its majority and minority carriers. In particular we found that the carrier recombination in single-phase hydrogenated microcrystalline silicon ($μ$c-Si:H) is significantly different from the one in hydrogenated amorphous silicon (a-Si:H) and that it is controlled only by its two band tails. Th e comparison of the observed temperature dependence of the phototransport properties of this material with model simulations further suggests that, while the conduction-band tail has an exponential distribution of states, the valence-band-tail states have a Gaussian-like distribution. This, in turn, meets the challenge of the determination of the analytical shape of the density of states distribution from experimental data. Our experimental procedure implies then that this distribution is associated with the route through which the transport and phototransport take place and thus we conclude that both the recombination and transport in undoped single-phase $μ$c-Si:H take place in the disordered layer that wraps the crystallites. We further conclude that, from the transport and phototransport points of view, the single-phase $μ$c-Si:H is, in general, different from both polycrystalline silicon and a-Si:H. The polycrystalline-silicon-like behavior, when found, appears to be an asymptotic case in which the crystallites are large enough, while the a-Si:H behavior prevails only when there is a significant content of its phase within the system.