{ "id": "1901.07025", "version": "v1", "published": "2019-01-21T18:31:16.000Z", "updated": "2019-01-21T18:31:16.000Z", "title": "Inverse-Compton emission from Millisecond Pulsars in the Galactic bulge", "authors": [ "Deheng Song", "Oscar Macias", "Shunsaku Horiuchi" ], "comment": "13 pages, 8 figures, 3 tables, submitted to PRD", "categories": [ "astro-ph.HE", "astro-ph.GA", "hep-ph" ], "abstract": "Analyses of $\\textit{Fermi Gamma-Ray Space Telescope}$ data have revealed a source of excess diffuse gamma rays towards the Galactic center that extends up to roughly $\\pm 20$ degrees in latitude. The leading theory postulates that this GeV excess is the aggregate emission from a large number of faint millisecond pulsars (MSPs). The electrons and positrons ($e^{\\pm}$) injected by this population could produce detectable inverse-Compton (IC) emissions by up-scattering ambient photons to gamma-ray energies. In this work, we calculate such IC emissions using $\\texttt{GALPROP}$. A triaxial 3D model of the bulge stars obtained from a fit to infrared data is used as a tracer of the putative MSP population. This model is compared against one in which the MSPs are spatially distributed as a Navarro-Frenk-White squared profile. We show that the resulting spectra for both models are indistinguishable, but that their spatial morphologies have salient recognizable features. The IC component above $\\sim $ TeV energies carry information on the spatial morphology of the injected $e^\\pm$. Such differences could potentially be used by future high-energy gamma-ray detectors such as Cherenkov Telescope Array (CTA) to provide a viable multiwavelength handle for the MSP origin of the GeV excess.", "revisions": [ { "version": "v1", "updated": "2019-01-21T18:31:16.000Z" } ], "analyses": { "keywords": [ "galactic bulge", "inverse-compton emission", "spatial morphology", "excess diffuse gamma rays", "tev energies carry information" ], "note": { "typesetting": "TeX", "pages": 13, "language": "en", "license": "arXiv", "status": "editable" } } }