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arXiv 2302.05026astro-ph.HEastro-ph.GA
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喷流功率、内禀$γ$射线光度和喷流AGN的吸积

Jet power, intrinsic $γ$-ray luminosity and accretion in jetted AGN

Chen Yonhyun, Gu Qiusheng, Fan Junhui, Yu xiaoling, Ding Nan, Guo Xiaotong, Xiong Dingrong

摘要:

动力学喷流功率$P_{\rm jet}$、内禀$γ$射线光度($L^{\rm int}$)和吸积($L_{\rm disk}$)之间的相关性可以揭示各种黑洞系统中的喷流物理。本文利用大量的喷流活动星系核样品,包括平谱射电类星体(FSRQs)、BL Lacertae天体(BL Lacs)、γ射线窄线Seyfert 1星系($γ$ NLS 1)和射电星系,研究了动力喷流功率、内禀$γ$射线光度和吸积之间的关系。主要结果如下:(1)全样本的$P_{\rm jet}$和$L^{\rm int}$之间关系的斜率指数分别为$0.85\pm0.01$,FSRQ的斜率指数为$0.70\pm0.02$,BL Lac的斜率指数为$0.83\pm0.03$,$γ$ NLS 1的斜率指数为$0.68\pm0.11$,射电星系的斜率指数为$0.93\pm0.09$。$γ$ NLS 1和射电星系中的喷流几乎遵循与费米耀变体相同的$P_{\rm jet}$ - $L^{\rm int}$关联。(2)$L^{\rm int}$和$L_{\rm disk}$之间关系的斜率指数分别为整个样本的$1.05\pm0.02$、FSRQ的$0.94\pm0.05$、BL Lac的$1.14\pm0.05$和$γ$ NLS 1的$0.92\pm0.18$。$γ$ NLS 1和射电星系几乎也遵循费米耀变体的$L^{\rm int}$ - $L_{\rm disk}$关联。(3)几乎所有喷流活动星系核的喷流功率都大于吸积盘的光度。喷流的能量取决于爱丁顿比和黑洞质量。我们得到了整个样本的$\log P_{\rm jet}\sim(1.00\pm0.02)\log L_{\rm disk}$,这与理论预测的系数是一致的。这些结果可能意味着喷流活动星系核的喷流是由Blandford-Znajek机制驱动的。

英文摘要:

The correlation between the kinetic jet power $P_{\rm jet}$, intrinsic $γ$-ray luminosity ($L^{\rm int}$) and accretion ($L_{\rm disk}$) may reveal the underlying jet physics in various black hole systems. We study the relation between kinetic jet power, intrinsic $γ$-ray luminosity, and accretion by using a large sample of jetted AGN, including flat-spectrum radio quasars (FSRQs), BL Lacertae objects (BL Lacs), gamma-ray Narrow-line Seyfert 1 galaxies ($γ$NLS1s) and radio galaxies. Our main results are as follows: (1) The slope indices of the relation between $P_{\rm jet}$ and $L^{\rm int}$ are $0.85\pm0.01$ for the whole sample, $0.70\pm0.02$ for the FSRQs, $0.83\pm0.03$ for the BL Lacs, $0.68\pm0.11$ for the $γ$NLS1s, and $0.93\pm0.09$ for the radio galaxies, respectively. The jets in $γ$NLS1s and radio galaxies almost follow the same $P_{\rm jet}$-$L^{\rm int}$ correlation that was obtained for Fermi blazars. (2) The slope indices of the relation between $L^{\rm int}$ and $L_{\rm disk}$ are $1.05\pm0.02$ for the whole sample, $0.94\pm0.05$ for the FSRQs, $1.14\pm0.05$ for the BL Lacs, and $0.92\pm0.18$ for the $γ$NLS1s, respectively. The $γ$NLS1s and radio galaxies almost also follow the $L^{\rm int}$-$L_{\rm disk}$ correlation derived for Fermi blazars. (3) The jet power is larger than the luminosity of accretion disks for almost all jetted AGN. Jet power depends on both the Eddington ratio and black hole mass. We obtain $\log P_{\rm jet}\sim(1.00\pm0.02)\log L_{\rm disk}$ for the whole sample, which is consistent with the theoretically predicted coefficient. These results may imply that the jets of jetted AGN are powered by the Blandford-Znajek mechanism.

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