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Brazilian Journal of Physics

Print version ISSN 0103-9733On-line version ISSN 1678-4448

Braz. J. Phys. vol.37 no.1a São Paulo Mar. 2007 

Dark matter halos and the anisotropy of ultra-high energy cosmic rays in the Pierre Auger observatory



Beatriz B. SiffertI; B. LazarottoI; J. R. T. de Mello NetoI; Angela OlintoII

IInstituto de Física, Universidade Federal do Rio de Janeiro, Caixa Postal 68528, 21941-972, Rio de Janeiro, RJ, Brazil
IIDepartment of Astronomy and Astrophysics, Kavli Institute for Cosmological Physics, The University of Chicago, 5640 S. Ellis Ave. Chicago, IL 60637, U.S.A.




We analyze the cosmic ray arrival direction map that would be observed if the source of ultra high energy cosmic rays were the decay of dark matter particles in the halos of our galaxy and of the Andromeda galaxy (M31). To model the dark matter distribution throughout the halos we use two different density profiles, the Moore et al. and the Navarro-Frenk-White profile. The results show what would be seen by the Pierre Auger experiment, since we take into account its exposure. We evaluate the dipole and quadrupole terms for the resulting maps in the two density profiles cases and compare them with the terms expected for an isotropic sky.

Keywords: Dark matter; Ultra-high energy cosmic rays; Pierre Auger experiment




The origin of ultrahigh energy cosmic rays, that reach us with energy ~ 1020 eV, is still a matter of intense investigation. Until today cosmic ray experiments were not able to collect enough data in order to achieve any conclusions because the flux at these energies is extremely low [1].

The Pierre Auger observatory [2] will consist of two separate sites, one in Argentina and the other in the US, covering the whole sky with an exposure of about 105 for the southern instrument and about 106 for both observatories. Presently the southern instrument is being built in Argentina and should be completed by 2007. It will set new standards for the ultra high energy cosmic rays physics, since it will collect a much bigger amount of data than all previous experiments combined. In particular, it will probably be able to determine if ultra high energy cosmic rays come isotropically from all directios of the sky or if distinct point sources or other patterns exist.

During the propagation of cosmic rays from their source to us, they interact with the cosmic microwave background radiation. If the cosmic ray has energy above the threshold energy, 5×1019 eV, this interaction results in the photo-production of pions. The cosmic ray will lose energy through this process and theoretical predictions tell us that if it is detected with an energy higher than the threshold energy, it is likely that it would have come from a source ~ 102 Mpc distant from us [3], [4]. This is called GZK cutoff and it tells us that potential sources must be close to the Milky Way.

The idea that ultrahigh energy cosmic rays can originate from the decay of super-heavy dark matter particles in the halo of our galaxy and nearby galaxies becomes then very attractive, since potential astrophysical sources are very rare in our neighborhood. There are different candidates for dark matter particles as well as for their possible decay products. If the latter are photons, recent results obtained by the Pierre Auger collaboration [5] show that its data still allows the possibility that cosmic rays are generated through the decay of dark matter particles.

In this paper, we study the anisotropy patterns that would be observed by the Pierre Auger observatory (North and South sites) if cosmic rays come from the decay of dark matter particles in the halo of the Galaxy and in the halo of the Andromeda galaxy (M31) [6], [7]. For now, we make no assumptions about the nature of these particles.



Our analysis strongly depend on how we assume the dark matter particles are distributed throughout the halo. There exist several density profiles derived from high resolution N-body simulations that describe this distribution. We chose to use the Navarro-Frenk-White [8], hereafter NFW, and the Moore et al. [9], [10] profiles, which are believed to be the most accurate ones. They can be parametrized by the following expression [11]:

where r is the distance from the center of the galaxy to the halo element, r(0) is the distance from the center of the galaxy to the sun, r0 = r(r0) and the constants a, b and g take the values shown in Table 1.




Since the Earth is not located in the center of our galaxy, we expect that cosmic rays coming from the decay of dark matter particles would not be isotropic in their arrival direcitons. We define q as the angle between the galactic plane and the direction connecting the Earth and the dark matter element. The cosmic ray flux due to our galaxy's halo coming from that direction is given by:

where K depends on the model adopted for the dark matter particle and s is the distance between the Earth and the dark matter element.

If we assume that the dark matter halo of M31 follows the same density profile, the flux of cosmic rays observed on Earth coming from M31 will be [12]:

where z ~ 2 is the ratio between the masses of M31's halo and our galaxy's halo and D ~ 670 kpc is the distance to M31.



All events detected by the Auger observatory are subjected to its experimental exposure. The exposure gives the probability that a cosmic ray coming from a given direction of the sky will be detected. For very energetic cosmic rays, this probability actually depends only on the declination coordinate of the cosmic ray direction.

The map that would be observed by the north and the south sites of Auger if sources were distributed isotropically in the sky is shown in Fig 1, in galactic coordinates.



We can see that it is very important that the exposure is determined with the highest precision posible, since its paterns could be easily mistaken for an inexistent anisotropy.



A. Dark Matter Contribution

The cosmic ray arrival directions maps that would be observed by Auger if we assume that all cosmic rays come from decay of dark matter particles from both our galaxy and M31 can be seen in Fig 2 and Fig 3. We can see what would be detected if both halos follow the NFW or the Moore et al. profile.





We can see that, while both maps show an insignificant contribution of M31's halo, the NFW density profile assumption makes M31 brighter than than it is if we use the Moore et al. profile.

B. Adding an Isotropic Background

We now define the total flux of cosmic rays as the sum of a dark matter contribution and a flat background (all passing through the Auger's exposure):

We can then control the intensity of the background in our simulations by changing the value of the h factor.

Results for the two profiles and two different values of h are shown in Figs 4, 5, 6 and 7. We see that the dark matter contribution to all these maps (the bright spot in the center) is very low compared to the exposure effects induced on the background, even for a very high value of h = 0.2. Also, for all the maps produced, the contribution of M31 is visually inexistent.









We do not expect however a very high conribution from the galactic center, such as the one being represented by the case h = 0.2. If this contribution really existed, it would have already been seen by other experiments. The contribution we are expecting to see should be much fainter.

C. Angular Power Spectrum

In order to quantify the deviation from isotropy of the maps we produced, we chose to measure its angular power spectrum.

We can expand the cosmic ray intensity function over the sphere in the base of the spherical harmonics [13]:

where N is the total number of cosmic rays detected.

We define then the angular power spectrum as:

For all the maps obtained we calculated the dipole and quadrupole terms for different values of h. These results are shown in Figs 8 and 9.





We see that deviation from the isotropic case can be detected even for the lowest values of h. We chose to run the simulations until h = 0.2 because we saw from the previous results that in this case the contribution from our galaxy is already too strong compared to what we expected from the available data.

Those results cannot however be pomptly interpreted as a real dipole or quadrupole on the sky because they are ''disguised'' by the exposure effects. In order to quantify multiple intensities, one should subtract the exposure from the maps. This can be easely understood if we notice that, if those results reflected real dipole or quadrupoles, the points representing the backgroung should be zero throughout the x axis.



The results obtained in this work, although very preliminary, indicate that signatures of cosmic rays produced by dark matter decays may be hard to see. Even for cases in which the signal from dark matter origin is big compared with the background, the galactic center is very faint, if exposure subtraction is not done properly. The contribution of M31's halo is insignificant when compared to our galaxy's contribution.

An interesting extension of this study would be the analysis of the case in which not the decay, but the anihilation of dark matter particles in the halos of galaxys were the responsible for the creation of ultra high energy cosmic rays. In this case, our's galaxy contribution would have the flux:

where the only difference from equation 2 is the fact that the density is now squared. The same would apply to M31's halo and equation 3 would become

This anihilation scenario may be theoreticaly more plausible than the decay one because it doesn't impose a specfic lifetime for dark matter particles. On the other hand, it would predict a stronger signal from the center of our galaxy that, as aforemenioned, was already not seen by previous experiments.


[1] Cosmic rays: the most energetic particles in the universe, J.W. Cronin, Rev. Mod. Phys. 71, 165 (1999).         [ Links ]

[2] J. Abraham et al., P. Auger Collaboration, Nucl. Instrum. Meth. A 523, 50 (2004).         [ Links ]

[3] K. Greisen, Phys. Rev. Lett 16, 748 (1966).         [ Links ]

[4] G.T. Zatsepin and V. A. Kuzmin, JETP Lett. 4, 78 (1966).         [ Links ]

[5] Lecture given at the International School of Cosmic Ray Astrophysics - 15th Course: Ästrophysics at Ultra-high Energies", Erice, Italy, 20-27 June 2006.         [ Links ]

[6] G. Medina Tanco, A.A. Watson, Astropart. Phys. 12, 25 (1999).         [ Links ]

[7] W. Evans, F. Ferrer, and S. Sarkar, Astropart. Phys. 17, 319 (2002).         [ Links ]

[8] J.F. Navarro, C.S. Frenk, and S.D.M. White, ApJ, 490, 493 (1997).         [ Links ]

[9] B. Moore, Nature, 370, 629 (1994).         [ Links ]

[10] R. Flores, J.R. Primack, ApJ, 427, L1 (1994).         [ Links ]

[11] A.V. Kravtsov, A.A. Klypin, J.S. Bullock, and J.S. Primack, The Astrophysical Journal, 502, 48 (1998).         [ Links ]

[12] S.L. Dubovsky, P.G. Tinyakov, JETP Lett. 68, 107 (1998).         [ Links ]

[13] P. Sommers, Astropart. Phys. 14, 271 (2001).        [ Links ]



Received on 29 September, 2006

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