Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                

Search for dark matter cosmic-ray electrons and positrons from the Sun with the Fermi Large Area Telescope

A. Cuoco, P. De La Torre Luque, F. Gargano, M. Gustafsson, F. Loparco, M. N. Mazziotta, and D. Serini
Phys. Rev. D 101, 022002 – Published 13 January 2020

Abstract

We use 7 years of electron and positron Fermi-LAT data to search for a possible excess in the direction of the Sun in the energy range from 42 GeV to 2 TeV. In the absence of a positive signal we derive flux upper limits which we use to constrain two different dark matter (DM) models producing e+e fluxes from the Sun. In the first case we consider DM model being captured by the Sun due to elastic scattering and annihilation into e+e pairs via a long-lived light mediator that can escape the Sun. In the second case we consider instead a model where DM density is enhanced around the Sun through inelastic scattering and the DM annihilates directly into e+e pairs. In both cases we perform an optimal analysis, searching specifically for the energy spectrum expected in each case, i.e., a boxlike shaped and linelike shaped spectrum respectively. No significant signal is found and we can place limits on the spin-independent cross section in the range from 1046cm2 to 1044cm2 and on the spin-dependent cross section in the range from 1043cm2 to 1041cm2. In the case of inelastic scattering the limits on the cross section are in the range from 1043cm2 to 1041cm2. The limits depend on the life time of the mediator (elastic case) and on the mass splitting value (inelastic case), as well as on the assumptions made for the size of the deflections of electrons and positrons in the interplanetary magnetic field.

  • Figure
  • Figure
  • Figure
  • Figure
  • Figure
  • Figure
  • Received 30 August 2019

DOI:https://doi.org/10.1103/PhysRevD.101.022002

© 2020 American Physical Society

Physics Subject Headings (PhySH)

  1. Research Areas
Gravitation, Cosmology & Astrophysics

Authors & Affiliations

A. Cuoco1,2,6,7,*, P. De La Torre Luque3,4, F. Gargano3, M. Gustafsson5, F. Loparco3,4,†, M. N. Mazziotta3,‡, and D. Serini3,4

  • 1RWTH Aachen University, Institute for Theoretical Particle Physics and Cosmology (TTK), D-52056 Aachen, Germany
  • 2Université Grenoble Alpes, USMB, CNRS-Laboratoire d’Annecy de Physique des Particules, 9 Chemin de Bellevue, F-74940 Annecy, France
  • 3Istituto Nazionale di Fisica Nucleare, Sezione di Bari, via Orabona 4, I-70126 Bari, Italy
  • 4Dipartimento di Fisica “M. Merlin” dell’Università e del Politecnico di Bari, via Amendola 173, I-70126 Bari, Italy
  • 5Georg-August University Göttingen, Institute for theoretical Physics-Faculty of Physics, Friedrich-Hund-Platz 1, D-37077 Göttingen, Germany
  • 6Istituto Nazionale di Fisica Nucleare, Sezione di Torino, via Pietro Giuria 1, I-10125 Torino, Italy
  • 7Dipartimento di Fisica, Università di Torino, via P. Giuria 1, 10125 Torino, Italy

  • *cuoco@physik.rwth-aachen.de
  • francesco.loparco@ba.infn.it
  • mazziotta@ba.infn.it

Article Text (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 101, Iss. 2 — 15 January 2020

Reuse & Permissions
Access Options
CHORUS

Article Available via CHORUS

Download Accepted Manuscript
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1

    Probability that CREs produced in the decays of a mediator travelling from the Sun to the Earth can reach the Earth as a function of the decay length of the mediator.

    Reuse & Permissions
  • Figure 2
    Figure 2

    Capture rate as a function of the DM mass, for the spin independent (blue line) and spin dependent (red line) cases. In both cases a scattering cross section of 1040cm2 is assumed.

    Reuse & Permissions
  • Figure 3
    Figure 3

    Number of events as a function of the observed energy for RoIs of 2° (black), 5° (red), 10° (blue), 30° (magenta), and 45° (green). Full circles: Sun RoIs; open circles: anti-Sun RoIs. The histograms are divided in 64 bins per energy decade. The error bars correspond to the square root of the number of events in each bin.

    Reuse & Permissions
  • Figure 4
    Figure 4

    Results of the search for boxlike features in 10° (left column), 30° (middle column), and 45° (right column) RoIs. The first row shows the upper limit at 95% CL on the line intensity compared with the expectations from the pseudoexperiments (the green and yellow bands show the central 68% and 95% expectation bands for the 95% CL limit). The second row shows the value of the local TS in the various energy windows compared with the expectations from the pseudoexperiments (the green and yellow bands show the one-sided 68% and 95% expectation bands for the local TS). The third row shows the conversion from the local TS to the global significance. The last row shows the upper limits on the DM-nucleon cross section for both the spin-dependent and spin-independent cases for four different decay length for the long-lived mediator L=R, 0.1, 1, and 5 AU. The plots also show the limits at 90% CL from the PICO-60 experiment [40] in the case of spin-dependent (SD) scattering (cyan line) and from the XENON1T experiment [41] in the case of spin-independent (SI) scattering (blue line).

    Reuse & Permissions
  • Figure 5
    Figure 5

    Results of the search for linelike features in 10° (left column), 30° (middle column), and 45° (right column) RoIs. The first row shows the upper limit at 95% CL on the line intensity compared with the expectations bands from the pseudoexperiments (the green and yellow bands show the central 68% and 95% expectation bands for the 95% CL limit). The second row shows the value of the local TS in the various energy windows compared with the expectations from the pseudoexperiments (the green and yellow bands show the one-sided 68% and 95% expectation bands for the TS local). The third row shows the conversion from the local TS to the global significance. The last row shows the upper limits on the cross section per nucleon σ0 for DM annihilation to e+e via inelastic scattering as a function of energy, calculated for three values of the splitting mass parameter, i.e., Δ=110, 125 and 140 keV.

    Reuse & Permissions
  • Figure 6
    Figure 6

    Upper limits at 95% CL on the spin-dependent DM-nucleon scattering cross section for the long lived mediator with decay length L=R. The current results with different RoIs, from 2 to 45°, are shown together with those from the HAWC and Fermi [44] with gamma rays from DM annihilating into 2 e±, i.e., 2 e± FSR γ case, (gray lines) and into 4γ (brown lines). The cyan line shows the PICO-60 limits at 90% CL [40].

    Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review D

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×