Data from the L3, Tasso, Opal and Delphi collaborations are analyzed in terms of a statistical model of high energy collisions. The model contains a power law critical exponentτ and Levy indexα . These data are used to study values ofτ andα . The very high multiplicity events in L3, Opal and Delphi are consistent with a model based on a Feynman-Wilson gas which has a tail exponentτ =3/2 and α =1/2. PAC number : 25.75. Dw, 24.10.Pa, 25.75.Gz Key words : critical exponents, particle multiplicity, Feynman-Wilson gas Phenomenological models of hadron multiplicities have been applied to understanding high energy collisions [1][2][3][4][5][6][7][8]. Several of these models are based on specific statistical models of photon count distributions [9,10]. These models were first used as probability distributions for event-by-event fluctuations in high energy collisions in small systems such as and in the past. Their use in large systems (heavy ion collisions) is gaining significant attention because of RHIC experiments. For example, large fluctuations in the neutral pion component are a property of a disoriented chiral condensate [11,12] and such fluctuations are being looked for in RHIC experiments. Past interest centered around dynamical theories which would produce large non-poissonian fluctuations seen in experimental data which could be interpreted in terms of fractal behavior and intermittency associated with a possible underlying cascade process. Two specific and frequently used models are the negative binomial model and a distribution based on photon emission from Lorentzian line shapes as initially developed by Glauber [13]. The latter model is also connected to a Feynman-Wilson gas as discussed in detail in ref [14,6] and briefly mentioned below. These two specific models have been extended in a previous paper [4,5,6] and shown to be special cases of a more general model. A main element of this more general model is a power law critical exponent( p e τ which appears in statistical physics, or a related Levy index α of probability theory. Various values ofτ orα distinguishes different models in our generalized approach which leads to a unified description of count distributions. Some connections of a Levy distribution with Bose-Einstein correlations and HBT features were also discussed in ref [15][16][17]. A physical interpretation was given in this reference where the fractal properties of a QCD cascade can be measured by a Levy index. In particular, if this cascade of particles arises