- th / 9 41 00 38 v 1 2 1 O ct 1 99 4 The Role of Final State Interactions in Quasielastic

ar X iv : n uc l - th / 9 60 80 59 v 1 2 8 A ug 1 99 6 DOE / ER / 40427 - 22 - N 96 Chiral Transparency

Color transparency is the vanishing of initial and final state interactions, predicted by QCD to occur in high momentum transfer quasielastic nuclear reactions. For specific reactions involving nucleons, the initial and final state interactions are expected to be dominated by exchanges of pions. We argue that these interactions are also suppressed in high momentum transfer nuclear quasielastic ...

- th / 9 41 10 04 v 1 7 N ov 1 99 4 COLOR TRANSPARENCY ASSUMPTIONS

An exactly solvable model is used to investigate the assumptions behind color transparency. 1 INTRODUCTION Color transparency (CT) is the anomalously high transparency of the nucleus to nucle-ons in quasi-elastic high-momentum transfer nuclear processes, measured with resolution good enough to insure that no " extra " pions are produced. This means that the ab-sorptive nuclear optical potential...

- th / 0 60 70 03 v 3 1 9 O ct 2 00 6 Final State Interaction Effects in the e + e − → NN̄ Process near Threshold

- th / 9 41 00 33 v 1 1 9 O ct 1 99 4 Correlations in a Many - Body Calculation of 11

A many-body calculation of Li is presented where the only input is the welltested, finite-range D1S effective interaction of Gogny. Pairing correlations are included in a constrained Hartree-Fock-Bogolyubov calculation, while long-range collective correlations are introduced using a GCM derived calculation. Correlations are found to play an important role in describing Li. A substantive underly...

ar X iv : n uc l - th / 9 31 00 28 v 1 2 1 O ct 1 99 3 An antiproton - proton partial - wave analysis