The Influence of High Multiplicities at RHIC on the Gamov Factor

dc.creatorAnchishkin, D. V.
dc.creatorZajc, W. A.
dc.creatorZinovjev, G. M.
dc.date1999-04-22
dc.date1999-04-23
dc.date.accessioned2026-07-07T05:43:03Z
dc.date.available2026-07-07T05:43:03Z
dc.descriptionThe corrections for two-pion correlations due to electromagnetic final-state interactions at high secondary multiplicities are investigated. The analysis is performed by solving the Schrödinger equation with a potential which is dictated by the multi-particle environment. Two different post-freeze-out scenarios are examined. First, for a uniformly spread environment of secondary particles, a screened Coulomb potential is exploited. It is shown that the presence of a static and uniform post-freeze-out medium results in a noticeable deviation from the standard Gamov factor. However, after going to a more realistic model of an expanding pion system, this conclusion changes drastically. We argue that the density of the secondary pions n_π(t,R), where R is a distance from the fireball, is bounded from above by n_π(t,R)\le const/R^2 for all times t. Then, a two-particle scalar potential which is found as a solution of the Maxwell equation for non-uniform medium replaces the screened one. Even this upper limit does not result in an essential deviation from the Gamov correction.
dc.description11 pages, 7 figures, minor text corrections are made
dc.identifierhttps://arxiv.org/abs/nucl-th/9904061
dc.identifierhttp://arxiv.org/abs/nucl-th/9904061
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/83165
dc.subjectNuclear Theory
dc.titleThe Influence of High Multiplicities at RHIC on the Gamov Factor
dc.typetext

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