An SNR passes through the following stages as it expands:2
There are three types of supernova remnant:
Remnants which could only be created by significantly higher ejection energies than a standard supernova are called hypernova remnants, after the high-energy hypernova explosion that is assumed to have created them.3
Supernova remnants are considered the major source of galactic cosmic rays.456 The connection between cosmic rays and supernovas was first suggested by Walter Baade and Fritz Zwicky in 1934. Vitaly Ginzburg and Sergei Syrovatskii in 1964 remarked that if the efficiency of cosmic ray acceleration in supernova remnants is about 10 percent, the cosmic ray losses of the Milky Way are compensated. This hypothesis is supported by a specific mechanism called "shock wave acceleration" based on Enrico Fermi's ideas, which is still under development.7
In 1949, Fermi proposed a model for the acceleration of cosmic rays through particle collisions with magnetic clouds in the interstellar medium.8 This process, known as the "Second Order Fermi Mechanism", increases particle energy during head-on collisions, resulting in a steady gain in energy. A later model to produce Fermi Acceleration was generated by a powerful shock front moving through space. Particles that repeatedly cross the front of the shock can gain significant increases in energy. This became known as the "First Order Fermi Mechanism".9
Supernova remnants can provide the energetic shock fronts required to generate ultra-high energy cosmic rays. Observation of the SN 1006 remnant in the X-ray has shown synchrotron emission consistent with it being a source of cosmic rays.10 However, for energies higher than about 1018 eV a different mechanism is required as supernova remnants cannot provide sufficient energy.11
It is still unclear whether supernova remnants accelerate cosmic rays up to PeV energies. The future telescope CTA will help to answer this question.
Discovery of most recent supernova in our galaxy May 14, 2008 http://chandra.harvard.edu/press/08_releases/press_051408.html ↩
Reynolds, Stephen P. (2008). "Supernova Remnants at High Energy". Annual Review of Astronomy and Astrophysics. 46 (46): 89–126. Bibcode:2008ARA&A..46...89R. doi:10.1146/annurev.astro.46.060407.145237. /wiki/Bibcode_(identifier) ↩
Lai, Shih-Ping; Chu, You-Hua; Chen, C.-H. Rosie; Ciardullo, Robin; Grebel, Eva K. (2001). "A Critical Examination of Hypernova Remnant Candidates in M101. I. MF 83". The Astrophysical Journal. 547 (2): 754–764. arXiv:astro-ph/0009238. Bibcode:2001ApJ...547..754L. doi:10.1086/318420. S2CID 14620463. /wiki/ArXiv_(identifier) ↩
K. Koyama; R. Petre; E.V. Gotthelf; U. Hwang; et al. (1995). "Evidence for shock acceleration of high-energy electrons in the supernova remnant SN1006". Nature. 378 (6554): 255–258. Bibcode:1995Natur.378..255K. doi:10.1038/378255a0. S2CID 4257238. https://zenodo.org/record/1233170 ↩
"Supernova produces cosmic rays". BBC News. November 4, 2004. Retrieved 2006-11-28. http://news.bbc.co.uk/2/hi/science/nature/3981619.stm ↩
"SNR and Cosmic Ray Acceleration". NASA Goddard Space Flight Center. Archived from the original on 1999-02-21. Retrieved 2007-02-08. https://web.archive.org/web/19990221015927/http://imagine.gsfc.nasa.gov/docs/features/topics/snr_group/cosmic_rays.html ↩
S.P. Reynolds (2011). "Particle acceleration in supernova-remnant shocks". Astrophysics and Space Science. 336 (1): 257–262. arXiv:1012.1306. Bibcode:2011Ap&SS.336..257R. doi:10.1007/s10509-010-0559-8. S2CID 118735190. /wiki/ArXiv_(identifier) ↩
E. Fermi (1949). "On the Origin of the Cosmic Radiation". Physical Review. 75 (8): 1169–1174. Bibcode:1949PhRv...75.1169F. doi:10.1103/PhysRev.75.1169. /wiki/Bibcode_(identifier) ↩
"Ultra-High Energy Cosmic Rays". University of Utah. Retrieved 2006-08-10. http://www.cosmic-ray.org/reading/uhecr.html ↩