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What can the 2008/10 broadband flare of PKS?1502+106 tell us? - Nuclear opacity, magnetic fields, and the location of γ rays

机译:PKS的2008/10宽带火炬2008/10宽带火炬怎么办?1502 + 106告诉我们? - 核不透明度,磁场和γ射线的位置

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Context. The origin of blazar variability, as seen from radio up to γ rays, is still a heavily debated matter, and broadband flares offer a unique testbed for developing a better understanding of these extreme objects. One of these energetic outbursts was detected by Fermi /LAT in 2008 from the blazar PKS?1502+106. The outburst was observed from γ rays down to radio frequencies. Aims. Through the delay between flare maxima at different radio frequencies, we study the frequency-dependent position of the unit-opacity surface and infer its absolute position with respect to the jet base. This nuclear opacity profile enables the jet’s magnetic field tomography. We also localize the γ -ray emission region and explore the flare production mechanism. Methods. The PKS?1502+106 radio flare is studied through single-dish flux density measurements at 12 frequencies in the range 2.64 to 226.5?GHz. To quantify the flare, we employ both a Gaussian process regression and a discrete cross-correlation function analysis. Results. We find that the light curve parameters (flare amplitude and cross-band delays) show a power-law dependence on frequency. Delays decrease with frequency, and the flare amplitudes increase up to about 43?GHz, and then decay. This behavior is consistent with the propagation of a shock downstream in the jet. The self-absorbed radio cores are located between approximately ten and four?pc from the jet base, and their magnetic field strengths range between 14 and 176?mG, at the frequencies 2.64 to 86.24?GHz. Finally, the γ -ray active region is located at (1.9 ± 1.1) ?pc away from the jet base.
机译:语境。从收音机直到γ光线看,Blazar变异性的起源仍然是一个巨大辩论的物质,宽带耀斑提供了一个独特的测试台,用于更好地了解这些极端物体。来自Blazar PKS的Fermi / Lat在Blazar PKS的情况下,Fermi / Lat检测到这些能量爆发之一.1502 + 106。从γ射线观察到爆发到无线电频率。目标。通过不同射频的闪光Maxima之间的延迟,我们研究了单位透明度表面的频率相关位置,并在射流上推断出绝对位置。这种核不透明度型材使JET的磁场断层扫描。我们还定位了γ-射线排放区域,并探索了耀斑生产机制。方法。 PKS?1502 + 106无线电耀斑通过在2.64至226.5范围内的12个频率下通过单碟磁通密度测量进行研究。为了量化耀斑,我们使用高斯过程回归和离散的互相关函数分析。结果。我们发现光曲线参数(闪光幅度和交叉带延迟)显示了频率的幂律依赖性。延迟用频率降低,爆发幅度增加到约43?GHz,然后衰减。这种行为与喷气机中的冲击的传播一致。自吸收的无线电芯位于射流底座的大约十和四个电池之间,并且它们的磁场强度在14到176Ω·mg之间,频率为2.64至86.24?GHz。最后,γ-射线有源区位于(1.9±1.1)距离喷射基底。

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