1987
DOI: 10.1038/329135a0
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Photon–photon pair production and the opacity of SN1987A to TeV and PeV γ-rays

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Cited by 12 publications
(2 citation statements)
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“…In the case of γ-ray production, a significant fraction of the γ-rays will interact by pair production with target nuclei in the shell and will not be observed. Also, during the first few months, TeV γ-rays could interact with radiation from the photosphere of the supernova [47]. By several days after the explosion, the radius of the photosphere becomes smaller than that of the SNR shell, where the neutrons interact, and continues to decrease in radius relative to the shell.…”
Section: Spectrum Of Neutrons From Photodisintegration Of Fe Nucleimentioning
confidence: 99%
“…In the case of γ-ray production, a significant fraction of the γ-rays will interact by pair production with target nuclei in the shell and will not be observed. Also, during the first few months, TeV γ-rays could interact with radiation from the photosphere of the supernova [47]. By several days after the explosion, the radius of the photosphere becomes smaller than that of the SNR shell, where the neutrons interact, and continues to decrease in radius relative to the shell.…”
Section: Spectrum Of Neutrons From Photodisintegration Of Fe Nucleimentioning
confidence: 99%
“…Such a pulsar and nebula will inevitably contribute Aux at other wavelengths as well, and more detailed modeling is required to decide whether it can also fit with the observed light curve, 'the independent (y-ray) evidence for radiogenic energy input, and so forth. (Berezinsky and Ginzberg, 1987;Honda andMori, 1987a, 1987b;Protheroe, 1987). There is at most very marginal evidence for a TeV flux of about 3X10 ergs/s at the time of the January soft-x-ray flare (Kifune, 1988 (Srinivasan, 1985).…”
mentioning
confidence: 98%