Hard-Te V BL Lac objects are newly identified populations of active galactic nuclei with the emittedγ-ray photons well above Te V energies.In this paper,we explain the multiwavelength emission of six Hard-Te V BL Lac...Hard-Te V BL Lac objects are newly identified populations of active galactic nuclei with the emittedγ-ray photons well above Te V energies.In this paper,we explain the multiwavelength emission of six Hard-Te V BL Lac objects by using a truncated conical emission region of the jet,where the electron distribution is obtained by numerically solving the evolution equation along the jet self-consistently.For comparison,we also apply the model to Mrk 421and Mrk 501,which are the potential candidates for the hard Te V emissions.We demonstrate that the model can satisfactorily reproduce the spectral energy distributions of eight sources,particularly of six Hard-Te V sources,where no extreme minimum Lorentz factor of the electron population is required.In contrast with Mrk 421 and Mrk 501,six Hard-Te V sources have rather low magnetization in emitting regions and high cutoff energies of the electron distributions.展开更多
基金the financial supports from the growth project of young scientific and technological talents in colleges and universities in Guizhou Province(Qianjiaohe-KY-Zi[2020]221)Scientific Research Foundation for Doctoral Program of Xingyi Normal University for Nationalities(20XYBS16)。
文摘Hard-Te V BL Lac objects are newly identified populations of active galactic nuclei with the emittedγ-ray photons well above Te V energies.In this paper,we explain the multiwavelength emission of six Hard-Te V BL Lac objects by using a truncated conical emission region of the jet,where the electron distribution is obtained by numerically solving the evolution equation along the jet self-consistently.For comparison,we also apply the model to Mrk 421and Mrk 501,which are the potential candidates for the hard Te V emissions.We demonstrate that the model can satisfactorily reproduce the spectral energy distributions of eight sources,particularly of six Hard-Te V sources,where no extreme minimum Lorentz factor of the electron population is required.In contrast with Mrk 421 and Mrk 501,six Hard-Te V sources have rather low magnetization in emitting regions and high cutoff energies of the electron distributions.
