Leptonic Origin of TeV Gamma-Ray Emission from Crab Nebula
ZHANG Li1,2, WEI Bing-Tao2, FANG Jun1
1Department of Physics, Yunnan University, Kunming 6500912National Astronomical Observatories/Yunnan Observatory, Chinese Academy of Sciences, PO Box 110, Kunming 650011
Leptonic Origin of TeV Gamma-Ray Emission from Crab Nebula
ZHANG Li1,2;WEI Bing-Tao2;FANG Jun1
1Department of Physics, Yunnan University, Kunming 6500912National Astronomical Observatories/Yunnan Observatory, Chinese Academy of Sciences, PO Box 110, Kunming 650011
摘要We study the nonthermal emission of the Crab nebula in the bands from radio to TeV γ-ray on a simplified time-dependent injection model. In this model, relativistic electrons in the Crab nebula consists of two components and their injected spectrum is a broken power law with different indices and a break energy. The relativistic electrons emit nonthermal photons through synchrotron and inverse Compton scattering off soft photon fields inside the nebula. The resulting spectrum calculated with the model is well consistent with the observed data ranging from radio to very high energy γ-rays for the Crab nebula, where the emission from radio to medium γ-rays is from electron's synchrotron emission, whereas the emission above ~100MeV primarily comes from the inverse Compton scattering of the relativistic electrons on synchrotron photons.
Abstract:We study the nonthermal emission of the Crab nebula in the bands from radio to TeV γ-ray on a simplified time-dependent injection model. In this model, relativistic electrons in the Crab nebula consists of two components and their injected spectrum is a broken power law with different indices and a break energy. The relativistic electrons emit nonthermal photons through synchrotron and inverse Compton scattering off soft photon fields inside the nebula. The resulting spectrum calculated with the model is well consistent with the observed data ranging from radio to very high energy γ-rays for the Crab nebula, where the emission from radio to medium γ-rays is from electron's synchrotron emission, whereas the emission above ~100MeV primarily comes from the inverse Compton scattering of the relativistic electrons on synchrotron photons.
[1] Weiler K W and Panagia N 1980 Astron. Astrophys. 90 269 [2] Rees M J and Gunn J E 1974 Mon. Not. R. Astron. Soc. 167 1 [3] Kennel C F and Coroniti F V 1984 Astrophys. J 283 694 Kennel C F and Coroniti F V 1984 Astrophys. J 283 710 [4] Wilson A S 1972 Mon. Not. R. Astron. Soc. 157 229 [5] Nolan P L et al 1993 Astrophys. J 409 710 [6] Weeks T C 1992 Space Sci. Rev. 59 315 [7] Aharonian F et al 2004 Astrophys. J 614 897 Aharonian F et al 2006 Astron. Astrophys. 457 899 [8] Atoyan A M and Aharonian F A 1996 Mon. Not. R. Astron.Soc. 278 525 [9] De Jager O C and Harding A K 1992 Astrophys. J 396 161 [10] Achterberg A, Gallant Y A, Kirk J G and Guthmann A W 2001 Mon. Not. R. Astron. Soc. 328 393 [11] Venter C and De Jager O C 2006 Proceedings of the 363WE-Heraeus Seminar on: Neutron Stars and Pulsars eds Becker W, Huang HH, MPE Report 291 p 40 [12] Kuiper L et al 2001 Astron. Astrophys. 378 918 [13] Baars J W M and Hartsuijker A P 1972 Astron. Astrophys. 17 172 [14] V\'eron-Cetty M P and Woltjer L 1993 Astron. Astrophys. 270 370 [15] Strom R G and Greidanus H 1992 Nature 358 654 [16] Bandiera R, Neri R and Cesaroni R 2002 Astron.Astrophys. 386 1044 [17] Green D A, Tuffs R J and Popescu C C 2004 Mon. Not. R.Astron. Soc. 355 1315 [18] Marsden P L et al 1984 Astrophys. J 278 L29