Critical fluctuations of the proton density in A+A collisions at 158A GeV

The method has been tested using events generated in the Cugnon cascade model C121, and has been found to reproduce well the results from the known direction of the reaction plane.

We report in this letter the first experimental evidence that close to the critical point of a second or- der phase transition, the PDF of a spatially averaged order parameter takes

The initial condition is the following: at time zero, each site in x ∈ Z bears a random number of particles whose distribution is Poisson with parameter ρ > 0, the.. Key words

On the transverse momentum distribution of strange hadrons produced in relativistic heavy ion collisions..

Finally, we acknowledge the enduring support for the construction and operation of the LHC and the CMS detector provided by the following funding agencies: the Austrian Federal

Figure 4.9: Realistic packet ordering - Comparison of the distribution of packet sizes (a, b, c), the number of packets per bidirectional flow (d, e, f), the number of bytes

If the atomic relaxation rate is fast compared to the Larmor frequency, then the nucleus cannot respond to the individual fields H, 0, and -H, and all nuclei experience the

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