Ultra-high-energy cosmic ray

Unsolved problems in physics
Why is it that some cosmic rays appear to possess energies that are theoretically too high?

In astroparticle physics, an ultra-high-energy cosmic ray (UHECR) or extreme-energy cosmic ray (EECR) is a cosmic ray with an extreme kinetic energy, far beyond both its rest mass and energies typical of other cosmic rays.

These particles are significant for astrophysics and fundamental physics theory, because they have energies comparable to the Greisen–Zatsepin–Kuzmin limit, which occurs at about 5×1019 electron volts (8 J). This limit should be the maximum energy of cosmic rays that have traveled long distances (about 160 million light years), due to the theoretical energy losses of higher-energy rays and to scattering from photons in the cosmic microwave background.

Contents

Observational history

The first observation of a cosmic ray with an energy exceeding 1.0×1020 eV (16 J) was made by Dr John D Linsley and Livio Scarsi at the Volcano Ranch experiment in New Mexico in 1962.[1][2]

Cosmic rays with even higher energies have since been observed. Among them was the Oh-My-God particle observed on the evening of 15 October 1991 over Dugway Proving Ground, Utah. Its observation was a shock to astrophysicists, who estimated its energy to be approximately 3×1020 eV (50 J)[3]—in other words, a subatomic particle with kinetic energy equal to that of a baseball (5 ounces or 142 grams) traveling at about 100 kilometers per hour (60 mph). It was most probably a proton traveling at about (1 − 5×10−24) metres per second slower than the speed of light (approximately 0.9999999999999999999999951c), so close that in a year-long race between light and the cosmic ray, the ray would fall behind only 46 nanometers (5×10−24 light-years), or 0.15 femtoseconds (1.5×10−16 s).[4]

The energy of this particle is some 40 million times that of the highest energy protons that can currently be produced in any terrestrial particle accelerator. However only a small fraction of this energy would be available for an interaction with a proton or neutron on Earth, with most of the energy remaining in the form of kinetic energy of the products of the interaction. The effective energy available for such a collision is the square root of double the product of the particle's energy and the mass energy of the proton, which for this particle gives 7.5×1014 eV, roughly 50 times the collision energy of the Large Hadron Collider.

Since the first observation, by the University of Utah's Fly's Eye Cosmic Ray Detector, at least fifteen similar events have been recorded, confirming the phenomenon. These very high energy cosmic rays are very rare; the energy of most cosmic rays is between 10 MeV and 10 GeV.

Active galactic cores as one possible source of the particles

Interactions with blue-shifted cosmic microwave background radiation limit the distance that these particles can travel before losing energy; this is known as the Greisen–Zatsepin–Kuzmin limit or GZK limit.

The source of such high energy particles has been a mystery for many years. Recent results from the Pierre Auger Observatory show that ultra-high-energy cosmic ray arrival directions appear to be correlated with extragalactic supermassive black holes at the center of nearby galaxies called active galactic nuclei (AGN).[5] However, since the angular correlation scale used is fairly large (3.1 degrees) these results do not unambiguously identify the origins of such cosmic rays. The AGN could merely be closely associated with the actual sources, for example in galaxies or other astrophysical objects that are clumped with matter on large scales within 100 Mpc.

Additional data collection is important for further investigating possible AGN sources for these highest energy particles.

Some of the supermassive black holes in AGN are known to be rotating, as in the Seyfert galaxy MCG 6-30-15[6] with time-variability in their inner accretion disks.[7] Black hole spin is a potentially effective agent to drive UHECR production,[8] provided ions are suitably launched to circumvent limiting factors deep within the nucleus, notably curvature radiation[9] and inelastic scattering with radiation from the inner disk. Low-luminosity, intermittent Seyfert galaxies may meet the requirements with the formation of a linear accelerator several light years away from the nucleus, yet within their extended ion tori whose UV radiation ensures a supply of ionic contaminants.[10] The corresponding electric fields are small, on the order of 10 V/cm, whereby the observed UHECRs are indicative for the astronomical size of the source. Improved statistics by the Pierre Auger Observatory will be instrumental in identifying the presently tentative association of UHECRs (from the Local Universe) with Seyferts and LINERs.[11]

Other possible sources of the particles

Other possible sources of the UHECR are:[12]

Relation with dark matter

Conversion of dark matter into ultra-high-energy particles

It is hypothesized that active galactic nuclei are capable of converting dark matter into high energy protons. Yuri Pavlov and Andrey Grib at the Alexander Friedmann Laboratory for Theoretical Physics at St. Petersburg hypothesize that dark matter particles are about 15 times heavier than protons, and that they can decay into pairs of particles of a type that interacts with ordinary matter.[13]

Near an active galactic nucleus, one of these particles can fall into the black hole, while the other escapes, as described by the Penrose process. Some of the particles that escape will collide with incoming particles creating collisions of very high energy. It is in these collisions, according to Pavlov, that ordinary visible protons can form. These protons would have very high energies. Pavlov claims that evidence of this is present in the form of ultra-high-energy cosmic rays.[14]

Ultra-high energy cosmic rays may also be produced by the decay of super-heavy dark matter "X particles" [15] such as Holeums.[16][17] Such very energetic decay products, carrying a fraction of the mass of the X particle, are believed to be a plausible explanation for the observed ultra-high energy cosmic rays (UHECR).

Dark matter particles as ultra-high-energy particles

High energy cosmic rays traversing intergalactic space suffer the GZK cutoff above 1020 eV due to interactions with cosmic background radiation if the primary cosmic ray particles are protons or nuclei. The Pierre Auger Project, HiRes and Yakutsk Extensive Air Shower Array found the GZK cutoff, while Akeno-AGASA observed the events above the cutoff (11 events in the past 10 years). The result of the Akeno-AGASA experiment is smooth near the GZK cutoff energy. If one assumes that the Akeno-AGASA result is correct and consider its implication, a possible explanation for the AGASA data on GZK cutoff violation would be a shower caused by dark matter particles. A dark matter particle is not constrained by the GZK cutoff, since it interacts weakly with cosmic background radiation. Recent measurements by the Pierre Auger Project have found a correlation between the direction of high energy cosmic rays and the location of AGN.[18]

Pierre Auger Observatory

Pierre Auger Observatory is an international cosmic ray observatory designed to detect ultra-high-energy cosmic rays (subatomic particles (protons or other nuclei) with energies beyond 1020 electron-volts). These high-energy particles have an estimated arrival rate of just 1 per square kilometer per century, therefore, in order to record a large number of these events, the Auger Observatory has created a detection area of 3,000 km² (the size of Rhode Island, USA) in Mendoza Province, western Argentina.

A larger cosmic-ray detector array is also planned for the northern hemisphere as part of the Pierre Auger complex.

The Pierre Auger Observatory, in addition to obtaining directional information from the cluster of water tanks used to observe the cosmic-ray-shower components, also has four telescopes trained on the night sky to observe fluorescence of the nitrogen molecules as the shower particles traverse the sky, giving further directional information on the original cosmic ray.

Ultra-high-energy cosmic ray observatories

See also

References

  1. ^ J. Linsley (1963). "Evidence for a Primary Cosmic-Ray Particle with Energy 1020 eV". Physical Review Letters 10 (4): 146. Bibcode 1963PhRvL..10..146L. doi:10.1103/PhysRevLett.10.146. 
  2. ^ physics world.com
  3. ^ Open Questions in Physics. German Electron-Synchrotron. A Research Centre of the Helmholtz Association. Updated March 2006 by JCB. Original by John Baez.
  4. ^ J. Walker (January 4, 1994). "The Oh-My-God Particle". Fourmilab. http://www.fourmilab.ch/documents/OhMyGodParticle/. 
  5. ^ The Pierre Auger Collaboration (November 9, 2007). "Correlation of the Highest-Energy Cosmic Rays with Nearby Extragalactic Objects". http://www.sciencemag.org/cgi/content/short/318/5852/938. 
  6. ^ Tanaka, Y., Nandra, K., Fabian, A.C., et al., 1995, Nature, 375, 659
  7. ^ Iwasawa, K., Fabian, A.C., Reynolds, C.S., et al., 1996, MNRAS, 282, 1038
  8. ^ Boldt, E., Gosh, P., 1999, MNRAS, 307, 491
  9. ^ Levinson, A., 2000, Phys. Rev. Lett., 85, 912
  10. ^ van Putten, M.H.P.M., Gupta, A.C., 2009, MNRAS, 394, 2238
  11. ^ Moskalenko, I.V., Stawarz, L., Porter, T.A., Cheung, C.-C., 2008, preprint (ArXiv:0805.1260)
  12. ^ Lofar - Astronomy
  13. ^ e-Print Archive - Active Galactic Nuclei and Transformation of Dark Matter into Visible Matter
  14. ^ e-Print archive - Do Active Galactic Nuclei Convert Dark Matter into Visible Particles?
  15. ^ e-Print Archive - Ultra-high energy cosmic rays from super-heavy X particle decay
  16. ^ e-Print Archive - L. K. Chavda and Abhijit Chavda - Dark matter and stable bound states of primordial black holes
  17. ^ e-Print Archive - L. K. Chavda and Abhijit Chavda - Ultra High Energy Cosmic Rays from decays of Holeums in Galactic Halos
  18. ^ e-Print archive - Search for a dark matter particle in high energy cosmic rays

Further reading

External links