2008
DOI: 10.1111/j.1745-3933.2008.00485.x
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MAGIC J0616+225 as delayed TeV emission of cosmic rays diffusing from the supernova remnant IC 443

Abstract: We present a theoretical model that explains the high-energy phenomenology of the neighbourhood of the supernova remnant IC 443, as observed with the Major Atmospheric Gamma Imaging Cherenkov (MAGIC) telescope and the Energetic Gamma-Ray Experiment Telescope (EGRET). We interpret MAGIC J0616+225 as delayed TeV emission of cosmic rays diffusing from IC 443 and interacting with a known cloud located at a distance of about 20 pc in the foreground of the remnant. This scenario naturally explains the displacement b… Show more

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Cited by 42 publications
(48 citation statements)
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References 50 publications
(70 reference statements)
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“…The diffusion radius for tT pp is R dif (E ) ¼ 2½D(E )t 1 = 2 , so that at a fixed age and distance, only particles of higher energy will be able to compensate for a smaller D 10 , producing SED maxima at higher E-values. The smaller values of D 10 that we study are expected in dense regions of the ISM (e.g., Ormes et al 1988;Torres et al 2008). It is interesting to note that for many, albeit not for all, of the SEDs studied, the maximum in E 2 F space is found at energies beyond the energetic range of GLAST.…”
Section: The Role Of Diffusionmentioning
confidence: 50%
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“…The diffusion radius for tT pp is R dif (E ) ¼ 2½D(E )t 1 = 2 , so that at a fixed age and distance, only particles of higher energy will be able to compensate for a smaller D 10 , producing SED maxima at higher E-values. The smaller values of D 10 that we study are expected in dense regions of the ISM (e.g., Ormes et al 1988;Torres et al 2008). It is interesting to note that for many, albeit not for all, of the SEDs studied, the maximum in E 2 F space is found at energies beyond the energetic range of GLAST.…”
Section: The Role Of Diffusionmentioning
confidence: 50%
“…We assume typical values, ¼ 2:2 and ¼ 0:5. In the case of energy-dependent propagation of CRs, a large variety of -ray spectra is expected (e.g., Aharonian & Atoyan 1996;Torres et al 2008). Diffusion of CRs has also been explored as an explanation for the high-energy observations of the Galactic center (e.g., Hinton & Aharonian 2007).…”
Section: The Role Of Diffusionmentioning
confidence: 99%
“…Here, as indicated in Figure 9 (left), there is no connection between n x and n γ because the X-rays are produced in the SNR shell while the γ-rays are from the MC. Such a scenario has been suggested to explain the γ-rays from the source MAGIC J0616+225 as the result of energetic particles that have escaped from IC 443 and are interacting with dense clouds (Torres et al 2008), for example, and discrete TeV sources outside the remnant W28 have been suggested to originate from particles escaping the SNR and interacting with adjacent clouds ). The expected γ-ray spectrum in this scenario is complicated, however.…”
Section: Gamma-ray Observations Of Snrsmentioning
confidence: 99%
“…For IC 443 the centroids of the GeV and TeV emission are not coinciding, a fact that could be explained as the result of the escape of high energy CRs from the SNR shell and of their interaction with the ambient medium. In this scenario, the diffusion coefficient for the multi-TeV CRs is of the order of D ≈ 10 27 ( CR/0.1) 2 cm 2 /s (with CR the efficiency of converting the SN explosion energy into CRs), a diffusion coefficient that is much smaller than the average diffusion coefficient in the Galaxy (75). While these measurement provide an important proof of the acceleration of CR protons in shock wave of SNRs, the lessons that can be learned on the acceleration of the bulk of CRs in our Galaxy are somewhat limited since the maximum particle energy is way short of the "knee" in the spectrum of CRs.…”
Section: The Origin Of Cosmic Raysmentioning
confidence: 99%