{"@context":"http://iiif.io/api/presentation/2/context.json","@id":"https://repo.library.stonybrook.edu/cantaloupe/iiif/2/manifest.json","@type":"sc:Manifest","label":"A Search for Charm and Beauty in a Very Strange \nWorld","metadata":[{"label":"dc.description.sponsorship","value":"This work is sponsored by the Stony Brook University Graduate School in compliance with the requirements for completion of degree."},{"label":"dc.format","value":"Monograph"},{"label":"dc.format.medium","value":"Electronic Resource"},{"label":"dc.identifier.uri","value":"http://hdl.handle.net/1951/59716"},{"label":"dc.language.iso","value":"en_US"},{"label":"dc.publisher","value":"The Graduate School, Stony Brook University: Stony Brook, NY."},{"label":"dcterms.abstract","value":"The Relativistic \nHeavy Ion Collider (RHIC) was built to produce and study the extremely hot and dense phase of matter called Quark \nGluon Plasma (QGP) in which the degrees of freedom are individual partons rather than composite hadrons. Since 2000, \nRHIC has collided various species of particles in order to disentangle and isolate the properties of the strongly \ninteracting QGP: p+p to set a baseline, d+Au to establish a control experiment, Au+Au to definitively create the QGP, \nand Cu+Cu to bridge the gap between d+Au and Au+Au. Electron-positron pairs are a particularly effective probe of \nthe QGP because they carry no color charge. Therefore, once created, these leptons do not interact strongly with the \nmedium. As a result, they retain characteristics of the full time evolution and dynamics of the system. There are \nmany features of interest in the dielectron invariant mass spectrum. The low mass region (m<1 GeV/c2) consists \nprimarily of pairs from Dalitz decays of light hadrons and direct decays of vector mesons that can be modified by the \nmedium, while the intermediate (1