{
  "annotation_id": "67dc3914-40f2-4dab-8cba-9e5735159a8a",
  "date_created": "2026-03-02T18:00:04.812000Z",
  "date_modified": "2026-03-02T18:00:04.812000Z",
  "file_hash": "bfb6f1ca25dc95e5363f5714a285f6f440245bea703d7f9198cc47e4b920acff",
  "private": false,
  "record": {
    "abstract": "We explicitly take into account the effect of hydrodynamic expansion profile\non the gluonic breakup of $J/\\psi$\u0027s produced in an equilibrating parton\nplasma. Attention is paid to the space-time inhomogeneities as well as Lorentz\nframes while deriving new expressions for the gluon number density $n_g$,\naverage dissociation rate $\u003c\\tilde{\\Gamma}\u003e$, and $\\psi$ survival probability\n$S$. A novel type of partial wave {\\em interference} mechanism is found to\noperate in the formula of $\u003c\\tilde{\\Gamma}\u003e$. Nonrelativistic longitudinal\nexpansion fro small length of the initial cylinder is found to push the\n$S(p_T)$ graph above the no flow case considered by us earlier \\cite{rev1}.\nHowever, relativistic flow corresponding to large length of the initial\ncylinder pushes the curve of $S(p_T)$ downwards at LHC but upwards at RHIC.\nThis mutually different effect on $S(p_T)$ may be attributed to the different\ninitial temperatures generated at LHC and RHIC.",
    "arxiv_id": "nucl-th/0503034",
    "authors": [
      "B. K. Patra",
      "V. J. Menon"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1140/epjc/s2005-02273-2",
    "journal_ref": "Eur.Phys.J.C44:567-576,2005",
    "title": "$J/\\psi$ Gluonic Dissociation Revisited : II. Hydrodynamic Expansion   Effects",
    "url": "https://arxiv.org/abs/nucl-th/0503034"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "4940b8db-ec39-484a-98b1-bc46ae7aa626",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}