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Based on observational data, the spectra of cosmic radio, microwave, infrared, optical, and x-ray photons are estimated. The absorption probability per unit path length by the process of pair production in photon-photon collisions is then computed as a function of energy for high-energy photons traversing this photon gas, using the results of the previous paper. These calculations show that there should be a dip in the intensity of the high-energy cosmic photon spectrum by about a factor of 10 between 10¹² and 10¹³ eV due to absorption by optical ({~} a few eV) photons. Above 10¹⁴ eV, the high-energy cosmic photon spectrum should essentially cut off because of the strong absorption by the cosmic 3^∘{}K blackbody photons, and at higher energies by the cosmic radio photons.
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Gould et al. (1967) studied this question.
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