650 research outputs found
Diffusive propagation of UHECR and the propagation theorem
We present a detailed analytical study of the propagation of ultra high
energy (UHE) particles in extragalactic magnetic fields. The crucial parameter
which affects the diffuse spectrum is the separation between sources. In the
case of a uniform distribution of sources with a separation between them much
smaller than all characteristic propagation lengths, the diffuse spectrum of
UHE particles has a {\em universal} form, independent of the mode of
propagation. This statement has a status of theorem. The proof is obtained
using the particle number conservation during propagation, and also using the
kinetic equation for the propagation of UHE particles. This theorem can be also
proved with the help of the diffusion equation. In particular, it is shown
numerically, how the diffuse fluxes converge to this universal spectrum, when
the separation between sources diminishes. We study also the analytic solution
of the diffusion equation in weak and strong magnetic fields with energy losses
taken into account. In the case of strong magnetic fields and for a separation
between sources large enough, the GZK cutoff can practically disappear, as it
has been found early in numerical simulations. In practice, however, the source
luminosities required are too large for this possibility.Comment: 16 pages, 13 eps figures, discussion of the absence of the GZK
cut-off in strong magnetic field added, a misprint in figure 6 corrected,
version accepted for publication in Ap
Disappointing model for ultrahigh-energy cosmic rays
Data of Pierre Auger Observatory show a proton-dominated chemical composition
of ultrahigh-energy cosmic rays spectrum at (1 - 3) EeV and a steadily heavier
composition with energy increasing. In order to explain this feature we assume
that (1 - 3) EeV protons are extragalactic and derive their maximum
acceleration energy, E_p^{max} \simeq 4 EeV, compatible with both the spectrum
and the composition. We also assume the rigidity-dependent acceleration
mechanism of heavier nuclei, E_A^{max} = Z x E_p^{max}. The proposed model has
rather disappointing consequences: i) no pion photo-production on CMB photons
in extragalactic space and hence ii) no high-energy cosmogenic neutrino fluxes;
iii) no GZK-cutoff in the spectrum; iv) no correlation with nearby sources due
to nuclei deflection in the galactic magnetic fields up to highest energies.Comment: 4 pages, 7 figures, the talk presented by A. Gazizov at NPA5
Conference, April 3-8, 2011, Eilat, Israe
Cosmic Rays from Cosmic Strings with Condensates
We re-visit the production of cosmic rays by cusps on cosmic strings. If a
scalar field (``Higgs'') has a linear interaction with the string world-sheet,
such as would occur if there is a bosonic condensate on the string, cusps on
string loops emit narrow beams of very high energy Higgses which then decay to
give a flux of ultra high energy cosmic rays. The ultra-high energy flux and
the gamma to proton ratio agree with observations if the string scale is GeV. The diffuse gamma ray and proton fluxes are well below current
bounds. Strings that are {\it lighter} and have linear interactions with
scalars produce an excess of direct and diffuse cosmic rays and are ruled out
by observations, while heavier strings ( GeV) are constrained by
their gravitational signatures. This leaves a narrow window of parameter space
for the existence of cosmic strings with bosonic condensates.Comment: 9 pages, 5 figures; revised reference
Signatures of Topological Defects
We argue that due to various restrictions cosmic strings and monopole-string
networks are not likely to produce the observed flux of ultra-high energy
cosmic rays (UHECR). Among the topological defects studied so far, the most
promising UHECR sources are necklaces and monopolonia. Other viable sources
which are similar to topological defects are relic superheavy particles. All
these sources have an excess of pions (and thus photons) over nucleons at
production. We demonstrate that in the case of necklaces the diffuse proton
flux can be larger than photon flux, due to absorption of the latter on
radiobackground, while monopolonia and relic particles are concentrated in the
Galactic halo, and the photon flux dominates. Another signature of the latter
sources is anisotropy imposed by asymmetric position of the sun in the Galactic
halo. In all cases considered so far, including necklaces, photons must be
present in ultra-high energy radiation observed from topological defects, and
experimental discrimination between photon-induced and proton-induced extensive
air showers can give a clue to the origin of ultra-high energy cosmic rays.Comment: version accepted for publication in Phys. Rev. D. No changes in the
conclusions and in figure
Neutrinos from Early-Phase, Pulsar-Driven Supernovae
Neutron stars, just after their formation, are surrounded by expanding,
dense, and very hot envelopes which radiate thermal photons. Iron nuclei can be
accelerated in the wind zones of such energetic pulsars to very high energies.
These nuclei photo-disintegrate and their products lose energy efficiently in
collisions with thermal photons and with the matter of the envelope, mainly via
pion production. When the temperature of the radiation inside the envelope of
the supernova drops below K, these pions decay before
losing energy and produce high energy neutrinos. We estimate the flux of muon
neutrinos emitted during such an early phase of the pulsar - supernova envelope
interaction. We find that a 1 km neutrino detector should be able to detect
neutrinos above 1 TeV within about one year after the explosion from a
supernova in our Galaxy. This result holds if these pulsars are able to
efficiently accelerate nuclei to energies eV, as postulated
recently by some authors for models of Galactic acceleration of the extremely
high energy cosmic rays (EHE CRs).Comment: 16 pages, 3 figures, revised version submitted to Ap
Astroparticle Physics: Puzzles and Discoveries
Puzzles often give birth to the great discoveries, the false discoveries
sometimes stimulate the exiting ideas in theoretical physics. The historical
examples of both are described in Introduction and in section ``Cosmological
Puzzles''. From existing puzzles most attention is given to Ultra High Energy
Cosmic Ray (UHECR) puzzle and to cosmological constant problem. The 40-years
old UHECR problem consisted in absence of the sharp steepening in spectrum of
extragalactic cosmic rays caused by interaction with CMB radiation. This
steepening is known as Greisen-Zatsepin-Kuzmin (GZK) cutoff. It is demonstrated
here that the features of interaction of cosmic ray protons with CMB are seen
now in the spectrum in the form of the dip and beginning of the GZK cutoff. The
most serious cosmological problem is caused by large vacuum energy of the known
elementary-particle fields which exceeds at least by 45 orders of magnitude the
cosmological vacuum energy. The various ideas put forward to solve this problem
during last 40 years, have weaknesses and cannot be accepted as the final
solution of this puzzle. The anthropic approach is discussed.Comment: Invited talk at TAUP 2007 conference, September 2007, Sendai, Japa
On the viability of holistic cosmic-ray source models
We consider the energy spectrum of cosmic-rays (CRs) from a purely
phenomenological point of view and investigate the possibility that they all be
produced by the same type of sources with a single power-law spectrum, in
E^{-x}, from thermal to ultra-high energies. We show that the relative fluxes
of the Galactic (GCR) and extra-galactic (EGCR) components are compatible with
such a holistic model, provided that the index of the source spectrum be x
\simeq 2.23\pm 0.07. This is compatible with the best-fit indices for both GCRs
and EGCRs, assuming that their source composition is the same, which is indeed
the case in a holistic model. It is also compatible with theoretical
expectations for particle acceleration at relativistic shocks.Comment: 5 pages, 1 figure, Accepted for publication in Astronomy and
Astrophysic
Galactic Anisotropy as Signature of ``Top-Down'' Mechanisms of Ultra-High Energy Cosmic Rays
We show that ``top-down'' mechanisms of Ultra-High Energy Cosmic Rays which
involve heavy relic particle-like objects predict Galactic anisotropy of
highest energy cosmic rays at the level of minimum . This anisotropy
is large enough to be either observed or ruled out in the next generation of
experiments.Comment: 8 pages, 1 figure, LaTeX. Final version appeared in Pisma Zh. Eksp.
Teor. Fi
Electroweak jet cascading in the decay of superheavy particles
We study decays of superheavy particles into leptons. We show that they
initiate cascades similar to QCD parton jets, if m_X\gsim 10^6 GeV.
Electroweak cascading is studied and the energy spectra of the produced leptons
are calculated in the framework of a broken SU(2) model of weak interactions.
As application, important for the Z-burst model for ultrahigh energy cosmic
rays, we consider decays of superheavy particles coupled on tree-level only to
neutrinos and derive stringent limit for these decays from the observed diffuse
extragalactic -ray flux.Comment: 4 pages, 1 eps figur
Bounds on the cosmogenic neutrino flux
Under the assumption that some part of the observed highest energy cosmic
rays consists of protons originating from cosmological distances, we derive
bounds on the associated flux of neutrinos generated by inelastic processes
with the cosmic microwave background photons. We exploit two methods. First, a
power-like injection spectrum is assumed. Then, a model-independent technique,
based on the inversion of the observed proton flux, is presented. The inferred
lower bound is quite robust. As expected, the upper bound depends on the
unknown composition of the highest energy cosmic rays. Our results represent
benchmarks for all ultrahigh energy neutrino telescopes.Comment: 12 pages, 6 figure
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