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arXiv 0710.0751astro-ph
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强子微类星体模型中的轻子二次发射

Leptonic secondary emission in a hadronic microquasar model

M. Orellana, P. Bordas, V. Bosch-Ramon, G. E. Romero, J. M. Paredes

摘要:

内容:有人提出,从具有喷流特征的高质量X射线双星(即所谓的微类星体(MQs))中发射的极高能量光子的起源与喷流中的相对论质子和星风中的冷质子之间的强子相互作用有关。轻子二次发射应该在一个完整的强子模型中计算,该模型包括喷注内部带电π衰变产生的对的影响和系统光球层中γ射线吸收产生的对的发射。目的:我们的目标是预测宽带谱从一般的强子微类星体模型,考虑到从秒的发射所产生的带电π衰变内喷流。方法:在考虑能量损失的情况下,一致地导出了沿喷注注入的次级轻子的粒子能量分布。在假设喷注内部磁场不同的情况下,我们还计算了这些轻子的光谱能量分布。中性π介子衰变产生的伽马射线在恒星光子场中经过电磁级联后的光谱。结果:我们发现,二次发射可以主导的光谱能量分布在低能量(~1 MeV)。在高能量下,电磁级联的影响会显著地扭曲产生谱。这些影响是相位相关的,并预测一些可变性调制的轨道周期。

英文摘要:

Context: It has been proposed that the origin of the very high-energy photons emitted from high-mass X-ray binaries with jet-like features, so-called microquasars (MQs), is related to hadronic interactions between relativistic protons in the jet and cold protons of the stellar wind. Leptonic secondary emission should be calculated in a complete hadronic model that include the effects of pairs from charged pion decays inside the jets and the emission from pairs generated by gamma-ray absorption in the photosphere of the system. Aims: We aim at predicting the broadband spectrum from a general hadronic microquasar model, taking into account the emission from secondaries created by charged pion decay inside the jet. Methods: The particle energy distribution for secondary leptons injected along the jets is consistently derived taking the energy losses into account. We also compute the spectral energy distribution resulting from these leptons is calculated after assuming different values of the magnetic field inside the jets. The spectrum of the gamma-rays produced by neutral pion-decay and processed by electromagnetic cascades under the stellar photon field. Results: We show that the secondary emission can dominate the spectral energy distribution at low energies (~1 MeV). At high energies, the production spectrum can be significantly distorted by the effect of electromagnetic cascades. These effects are phase-dependent, and some variability modulated by the orbital period is predicted.

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