We discuss as a new signature for the interaction of extragalactic ultrahigh energy protons with cosmic microwave background radiation a spectral feature located at $E=6.3\times 10^{19}$ eV in the form of a narrow and shallow dip. It is produced by the interference of $e^+e^-$-pair and pion production. We show that this dip and in particular its position are almost model-independent. Its observation by future ultrahigh energy cosmic ray detectors may give the conclusive confirmation that an observed steepening of the spectrum is caused by the Greisen-Zatsepin-Kuzmin effect
The temperature of the cosmic microwave background increases with redshift; at sufficiently high red...
We re-examine the interaction of ultra high energy nuclei with the microwave background radiation. W...
The spectrum of extra-galactic cosmic rays (CRs) is expected to follow the Greisen-Zatsepin-Kuzmin (...
A new feature in the spectrum of ultra high energy cosmic rays (UHECR) has been announced in the pap...
AbstractUltrahigh energy (UHE) extragalactic protons propagating through cosmic microwave radiation ...
Ultrahigh energy (UHE) extragalactic protons propagating through cosmic microwave radiation (CMB) ac...
Extragalactic cosmic ray protons with an injection spectrum of the type $E^{-2.7}$ show a spectrum o...
The dip is a feature in the diffuse spectrum of ultra-high energy (UHE) protons caused by electron-p...
We demonstrate that the energy spectra of Ultra High Energy Cosmic rays (UHECR) as observed by AGASA...
The dip is a feature in the diffuse spectrum of UHE protons in energy range $1\times 10^{18} - 4\tim...
We discuss the signatures of the transition from galactic to extragalactic cosmic rays in different ...
AbstractWe propose a scenario in which a simple power-like primary spectrum for protons with sources...
We re-examine the interaction of ultra high energy nuclei with the microwave background radiation. W...
The acceleration cites of ultra-high-energy (UHE) protons can be traced by the footprint left by the...
The clustering of ultra high energy (above 5\cdot 10^{19} eV) cosmic rays (UHECR) suggests that they...
The temperature of the cosmic microwave background increases with redshift; at sufficiently high red...
We re-examine the interaction of ultra high energy nuclei with the microwave background radiation. W...
The spectrum of extra-galactic cosmic rays (CRs) is expected to follow the Greisen-Zatsepin-Kuzmin (...
A new feature in the spectrum of ultra high energy cosmic rays (UHECR) has been announced in the pap...
AbstractUltrahigh energy (UHE) extragalactic protons propagating through cosmic microwave radiation ...
Ultrahigh energy (UHE) extragalactic protons propagating through cosmic microwave radiation (CMB) ac...
Extragalactic cosmic ray protons with an injection spectrum of the type $E^{-2.7}$ show a spectrum o...
The dip is a feature in the diffuse spectrum of ultra-high energy (UHE) protons caused by electron-p...
We demonstrate that the energy spectra of Ultra High Energy Cosmic rays (UHECR) as observed by AGASA...
The dip is a feature in the diffuse spectrum of UHE protons in energy range $1\times 10^{18} - 4\tim...
We discuss the signatures of the transition from galactic to extragalactic cosmic rays in different ...
AbstractWe propose a scenario in which a simple power-like primary spectrum for protons with sources...
We re-examine the interaction of ultra high energy nuclei with the microwave background radiation. W...
The acceleration cites of ultra-high-energy (UHE) protons can be traced by the footprint left by the...
The clustering of ultra high energy (above 5\cdot 10^{19} eV) cosmic rays (UHECR) suggests that they...
The temperature of the cosmic microwave background increases with redshift; at sufficiently high red...
We re-examine the interaction of ultra high energy nuclei with the microwave background radiation. W...
The spectrum of extra-galactic cosmic rays (CRs) is expected to follow the Greisen-Zatsepin-Kuzmin (...