2009
DOI: 10.1051/0004-6361/200809473
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Theory of cosmic ray and γ-ray production in the supernova remnant RX J0852.0-4622

Abstract: Aims. The properties of the Galactic supernova remnant (SNR) RX J0852.0-4622 are theoretically analysed.Methods. An explicitly time-dependent, nonlinear kinetic model of cosmic ray (CR) acceleration in SNRs is used to describe the properties of SNR RX J0852.0-4622, the accelerated CRs, and the nonthermal emission. The source is assumed to be at a distance of ≈1 kpc in the wind bubble of a massive progenitor star. An estimate of the thermal X-ray flux in this configuration is given. Results. We find that the ov… Show more

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Cited by 37 publications
(40 citation statements)
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References 78 publications
(176 reference statements)
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“…As a result, shock modification by the pressure gradient of the accelerating particles becomes possible everywhere on the shock surface. This reasoning follows the discussion in Berezhko et al (2009) with the conclusion that SNRs propagating into wind bubbles should have their forward shock modified everywhere. Technically, this implies that the SNR becomes spherically symmetric and the correction factor f re < 1 (Völk et al 2003) on the spherically symmetric solution reaches unity.…”
Section: Introductionsupporting
confidence: 76%
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“…As a result, shock modification by the pressure gradient of the accelerating particles becomes possible everywhere on the shock surface. This reasoning follows the discussion in Berezhko et al (2009) with the conclusion that SNRs propagating into wind bubbles should have their forward shock modified everywhere. Technically, this implies that the SNR becomes spherically symmetric and the correction factor f re < 1 (Völk et al 2003) on the spherically symmetric solution reaches unity.…”
Section: Introductionsupporting
confidence: 76%
“…We use the results of numerical calculations performed by Hamilton et al (1983) with some corrections. These mean that the X-ray emissivity of the remnant is reduced by the ratio R em = EM b /EM S of the emission measure EM b for our bubble solution to the emission measure for the classical Sedov solution EM S , which corresponds to a uniform ambient gas density N g (R s ) (Berezhko et al 2009). …”
Section: Estimate Of the Thermal X-ray Emissionmentioning
confidence: 94%
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“…This density profile was used by Berezhko & Völk (2006) and Berezhko et al (2009) for the case of RX J1713.7-3946 and Vela Jr., with n(r) = n b + (r/R b ) 3(σ sh −1) n sh , where n sh = σ sh n ICM is the maximum density of the shell at the outer boundary of the shell. In our work, we set σ sh = 5.…”
Section: Hess J1731-347 Evolving Into the Main-sequence Bubble Shellmentioning
confidence: 99%
“…Or, the known TeV-emitting shells no longer confine previously accelerated PeV (hadronic) particles; those particles would have escaped at earlier times of the SNR evolution and are at present already diffusing into the environment of the SNR. The latter hypothesis has been discussed in several works as a possibility to lower the high energy cutoff of TeV spectra of young SNRs in hadronically dominated TeV emission scenarios (e.g., Berezhko et al 2003;Malkov et al 2005;Berezhko et al 2009). …”
Section: Introductionmentioning
confidence: 99%