论文标题
Herschel Spire从射电射线射击的西部热点a发现了远红外的多余同步加速器排放
Herschel SPIRE discovery of far-infrared excess synchrotron emission from the west hot spot of the radio galaxy Pictor A
论文作者
论文摘要
射频和光度成像接收器(Spire)在板上赫切尔(Herschel)发现了射电星系A的西部热点的远红外对应物。源的颜色校正通量密度在350 $ $ m的波长下为$ 70.0 \ pm 9.9 $ mjy。对其无线电光谱进行的密切研究表明,用明智和spitzer检测到的无线电同步器组件上的中红外过量构成,对远红外带有显着贡献。多亏了SPIRE数据,据透露,多余的频谱由受到高能量截止的破碎幂律模型描述。通过在连续的能量注入($Δα= 0.5 $)下应用辐射冷却断裂,破碎的幂律模型支持了一个多余的想法,即多余的量子在热点范围内以10-PC量表子结构起源。 $ν_ {\ rm b} = 1.6 _ { - 1.0}^{+3.0} \ times 10^{12} $ hz,磁场估计为$ b \ simeq1 $ - $ 4 $ mg。这要高于子结构的最小能量磁场,高达$ 3 $ - $ 10 $。即使多余的原点大于$ \ sim 100 $ PC,也确认了比最小能源强的磁场。有人提出,通过血浆湍流局部增强的磁场的区域被视为子结构。突破以下的派生能量指数,$α\ sim 0.22 $(保守的$ <0.42 $),很难归因于强激加速度($α= 0.5 $)。随机加速度和磁重新连接被认为是合理的替代机制。
A far-infrared counterpart to the west hot spot of the radio galaxy Pictor A is discovered with the Spectral and Photometric Imaging REceiver (SPIRE) onboard Herschel. The color-corrected flux density of the source is measured as $70.0 \pm 9.9$ mJy at the wavelength of 350 $μ$m. A close investigation into its radio-to-optical spectrum indicates that the mid-infrared excess over the radio synchrotron component, detected with WISE and Spitzer, significantly contributes to the far-infrared band. Thanks to the SPIRE data, it is revealed that the spectrum of the excess is described by a broken power-law model subjected to a high-energy cutoff. By applying the radiative cooling break under continuous energy injection ($Δα= 0.5$), the broken power-law model supports an idea that the excess originates in 10-pc scale substructures within the hot spot. From the break frequency, $ν_{\rm b} = 1.6_{-1.0}^{+3.0} \times 10^{12}$ Hz, the magnetic field was estimated as $B\simeq1$-$4$ mG. This is higher than the minimum-energy magnetic field of the substructures by a factor of $3$--$10$. Even if the origin of the excess is larger than $\sim 100$ pc, the magnetic field stronger than the minimum-energy field is confirmed. It is proposed that regions with a magnetic field locally boosted via plasma turbulence are observed as the substructures. The derived energy index below the break, $α\sim 0.22$ (conservatively $<0.42$), is difficult to be attributed to the strong-shock acceleration ($α= 0.5$). Stochastic acceleration and magnetic reconnection are considered as a plausible alternative mechanism.