2019
DOI: 10.1103/physrevd.99.103016
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Hunting for superheavy dark matter with the highest-energy cosmic rays

Abstract: In 15 years of data taking the Pierre Auger Observatory has observed no events beyond 10 11.3 GeV. This null result translates into an upper bound on the flux of ultrahigh-energy cosmic rays implying J(> 10 11.3 GeV) < 3.6 × 10 −5 km −2 sr −1 yr −1 , at the 90%C.L. We interpret this bound as a constraint on extreme-energy photons originating in the decay super-heavy dark matter (SHDM) particles clustered in the Galactic halo. Armed with this constraint we derive the strongest lower limit on the lifetime of had… Show more

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Cited by 50 publications
(44 citation statements)
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“…As mentioned in the main body, rather than perform the DGLAP evolution from µ ∼ Q = m χ /2 down to µ ∼ q W , we instead start at the electroweak scale and evolve upwards. 11 In detail we start with q W = 100 GeV as the starting point for our evolution.…”
Section: B1 Review Of Dglap Evolution In the Unbroken Standard Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…As mentioned in the main body, rather than perform the DGLAP evolution from µ ∼ Q = m χ /2 down to µ ∼ q W , we instead start at the electroweak scale and evolve upwards. 11 In detail we start with q W = 100 GeV as the starting point for our evolution.…”
Section: B1 Review Of Dglap Evolution In the Unbroken Standard Modelmentioning
confidence: 99%
“…Heavy decaying DM can be realized in a number of different scenarios, including Wimpzillas [6][7][8][9][10][11], glueballs [12][13][14][15][16][17], gravitinos [18][19][20], superstring relics [21][22][23][24], and more recent proposals, see for example [25][26][27][28][29][30][31]. Independent of UV motivations, there is a clear reason to consider searching for such DM: the robust experimental program to probe astrophysical messengers at higher energies.…”
Section: Introductionmentioning
confidence: 99%
“…In general, one can distinguish two qualitatively different approaches in unveiling the physics of UHECRs: theoretical models assuming interactions of exotic super-heavy matter (including extra dimensions, Lorentz invariance violation, cosmic strings, existence of new particles etc. [68][69][70][71][72][73][74][75][76][77][78][79][80][81][82][83][84][85]) and acceleration scenarios describing processes, in which the particles are accelerated by a particular astrophysical object (shocks in relativistic plasma jets, unipolar induction mechanisms, second-order Fermi acceleration, etc.). Acceleration scenarios rely on the existence of powerful astrophysical sources with available energy that is sufficient for the energy transfer from these objects to cosmic-ray particles.…”
Section: Uhecr Sources and Cosmic-ray Ensemblesmentioning
confidence: 99%
“…In general, one can distinguish two qualitatively different approaches in unveiling the physics of UHECRs: theoretical models assuming interactions of exotic super-heavy matter (including extra dimensions, Lorentz invariance violation, cosmic strings, existence of new particles etc [69][70][71][72][73][74][75][76][77][78][79][80][81][82][83][84][85][86]) and acceleration scenarios describing processes, in which the particles are accelerated by a particular 1 The current experimental data suggests an extragalactic origin for UHECRs with energies above the GZK cutoff [63]. astrophysical object (shocks in relativistic plasma jets, unipolar induction mechanisms, second-order Fermi acceleration, etc.).…”
Section: Uhecr Sources and Cosmic Ray Ensemblesmentioning
confidence: 99%