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Distributions of Gamma-Ray Bursts and Blazars in the $L_{ m p}-E_{ m p}$ Plane and Possible Implications for their Radiation Physics

机译:$ L _ {\ rm p} -E _ {\ rm中的伽马射线爆发和爆炸的分布   p} $平面及其对辐射物理学的可能影响

摘要

We present a spectral analysis for a sample of redshift known GRBs observedwith {\em Fermi}/GBM. Together with the results derived from our systematicalspectral energy distribution modeling with the leptonic models for a {\emFermi}/LAT blazar sample, we compare the distributions of the GRBs and theblazars by plotting the synchrotron peak luminosity ($L_{\rm s}$) and thecorresponding peak photon energy $E_{\rm s}$ of blazars in the $L_{\rmp}-E_{\rm p}$ plane of GRBs, where $L_{\rm p}$ and $E_{\rm p}$ are the peakluminosity and peak photon energy of the GRB time-integrated $\nu f_\nu$spectrum, respectively. The GRBs are in the high-$L_{\rm p}$, high-$E_{\rm p}$corner of the plane and a tight $L_{\rm p}-E_{\rm p}$ relation is found, i.e.,$L_{\rm p}\propto E_{\rm p}^{2.13^{+0.54}_{-0.46}}$. Both FSRQs and LBLs areclustered in the low-$E_{\rm p}$, low-$L_{\rm p}$ corner. IBLs and HBLs have$E_{\rm s}\sim 2\times 10^{-3} - 10^{2}$ keV and $L_{\rm s} \sim 10^{44} -10^{47}$ erg s$^{-1}$, but no dependence of $L_{\rm s}$ on $E_{\rm s}$ isfound. We show that the tight $L_p-E_p$ relation of GRBs is potentiallyexplained with the synchrotron radiation of fast-cooling electrons in a highlymagnetized ejecta, and the weak anti-correlation of $L_{\rm s}-E_{\rm s}$ forFSRQs and LBLs may be attributed to synchrotron radiation of slow-coolingelectrons in a moderately magnetized ejecta. The distributions of IBLs and HBLsin the $L_{\rm p}-E_{\rm p}$ plane may be interpreted with synchrotronradiation of fast-cooling electrons in a matter-dominated ejecta. These resultsmay present a unified picture for the radiation physics of relativistic jets inGRBs and blazars within the framework of the leptonic synchrotron radiationmodels.
机译:我们提供了使用{\ em Fermi} / GBM观测到的已知红移GRB样本的光谱分析。结合我们使用{\ emFermi} / LAT blazar样本的轻子模型的系统光谱能量分布模型得出的结果,我们通过绘制同步加速器峰值光度($ L _ {\ rm s} $来比较GRB和Blazar的分布。 )和GRB的$ L _ {\ rmp} -E _ {\ rm p} $平面中对应的blazar峰值光子能量$ E _ {\ rm s} $,其中$ L _ {\ rm p} $和$ E _ {\ rm p} $分别是GRB时间积分$ \ nu f_ \ nu $光谱的峰值发光度和峰值光子能量。 GRB位于飞机的高$ L _ {\ rm p} $,高$ E _ {\ rm p} $ corner,并且紧密的$ L _ {\ rm p} -E _ {\ rm p} $关系是找到,即$ L _ {\ rm p} \ proto E _ {\ rm p} ^ {2.13 ^ {+ 0.54} _ {-0.46}} $。 FSRQ和LBL都聚集在低$ E _ {\ rm p} $,低$ L _ {\ rm p} $角。 IBL和HBL具有$ E _ {\ rm s} \ sim 2 \乘以10 ^ {-3}-10 ^ {2} $ keV和$ L _ {\ rm s} \ sim 10 ^ {44} -10 ^ {47 } $ erg s $ ^ {-1} $,但没有找到$ L _ {\ rm s} $对$ E _ {\ rm s} $的依赖性。我们表明,GRB的紧密的$ L_p-E_p $关系可以用强磁化喷射中的快速冷却电子的同步加速器辐射以及$ L _ {\ rm s} -E _ {\ rm s}的弱反相关来解释。 forFSRQ和LBL可能归因于中等磁化喷射中慢冷电子的同步加速器辐射。 $ L _ {\ rm p} -E _ {\ rm p} $平面中IBL和HBL的分布可以用物质主导的喷射中的快速冷却电子的同步辐射辐射来解释。这些结果可能为轻子同步加速器辐射模型框架内的GRBs和blazars的相对论射流的辐射物理学提供了一个统一的图景。

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