ar X iv : c s . C G / 9 91 10 13 v 1 2 8 N ov 1 99 9 PushPush is NP - hard in 3 D

ar X iv : c on d - m at / 9 81 14 09 v 1 2 9 N ov 1 99 8 Stripe phase ordering as quantum interference phenomenon

Stripe phase ordering as quantum interference phenomenon.

ar X iv : h ep - t h / 98 11 08 5 v 1 9 N ov 1 99 8 Vortex Solutions in the Chern - Simons Stuekelberg Model

ar X iv : c on d - m at / 9 61 11 80 v 1 2 3 N ov 1 99 6 Internal Forces and the Magnetoconductivity of a Nondegenerate 2 D Electron Fluid

X iv :c on dm at /9 61 11 80 v1 2 3 N ov 1 99 6 Internal Forces and the Magnetoconductivity of a Nondegenerate 2D Electron Fluid P. Fozooni, P.J. Richardson, and M.J. Lea Department of Physics, Royal Holloway, University of London, Egham, Surrey TW20 0EX, England M.I. Dykman and C. Fang-Yen[*] (a) Department of Physics and Astronomy, Michigan State University, MI 48824 (b) Department of Physics...

ar X iv : a st ro - p h / 99 11 43 8 v 1 2 3 N ov 1 99 9 H 2 molecules and cold clouds in cooling flow clusters †

ar X iv : c on d - m at / 9 91 14 28 v 1 2 6 N ov 1 99 9 The Values Distribution in a Competing Shares Financial Market Model

We present our competing shares financial market model and describe it's behaviour by numerical simulation. We show that in the critical region the distribution avalanches of the market value as defined in this model has a power-law distribution with exponent around 2.3. In this region the price returns distribution is truncated Levy stable.