论文标题
GEV $γ$ - 紧凑型陡峭光谱源4C +39.23b的排放
GeV $γ$-ray Emission of Compact Steep-Spectrum Source 4C +39.23B
论文作者
论文摘要
分析了4FGL J0824.9 +3915的13年观察数据,其中大面积望远镜在船上进行了Fermi Gamma Ray空间望远镜(Fermi/LAT)的分析,用于重新审视4C +39.23B,是否是紧凑型陡峭(CSS)源,是否封装到平面式QueSrum pecterrum pecterrum pecterrum pecterrum quassar(flats)。 $γ$ -RARE发射区域为4FGL J0824.9+3915,是$γ$ -Ray发射极。我们发现,4FGL J0824.9 +3915的时间集成$γ$ -Ray排放量由4C +39.23A压倒性地占主导地位。 It shows significant variability at a 6.7$σ$ confidence level and the average $γ$-ray flux in the 0.1--300 GeV energy band is $(1.60\pm 0.15)\times10^{-8}$ ph cm$^{-2}$ s$^{-1}$ with a power-law photon spectral index of $2.48\pm0.05$.在MJD 57500--58500期间,4FGL J0824.9+3915处于低状态,稳定的$γ$ ray助焊剂。 Analyzed the Fermi/LAT observation data in this time interval, it is found that the TS values of the $γ$-ray emission from 4C +39.23A and 4C +39.23B are $\sim5$ and $\sim 31$, respectively, indicating that the $γ$-ray emission in this time interval is dominated by the CSS 4C +39.23B. 4C +39.23b的此时间间隔中的派生平均通量为$(9.40 \ pm4.10)\ times 10^{ - 9} $ ph cm $^{ - 2} $ s $ s $^{ - 1} $,带有$γ_γ= 2.45 \ pm0.17 $。将4C +39.23B的光谱能分布(SED)归因于其核心和扩展区域的辐射,我们表明SED可以用两区Leptonic模型表示。它的$γ$射线排放由核心区域贡献。核心的衍生磁场强度和多普勒的增强因子为0.13 g和6.5。将4C +39.23B与其他$γ$ - 发射CSS和紧凑型对称对象(CSO)进行比较,在$γ_γ-L_γ$平面中,它类似于CSSS。
Thirteen yr observation data of 4FGL J0824.9+3915 with the Large Area Telescope on board the Fermi Gamma Ray Space Telescope (Fermi/LAT) are analyzed for revisiting whether 4C +39.23B, a compact steep-spectrum (CSS) source closed to a flat-spectrum radio quasar (FSRQ) 4C +39.23A in the $γ$-ray emitting region of 4FGL J0824.9+3915, is a $γ$-ray emitter. We find that the time-integrated $γ$-ray emission of 4FGL J0824.9+3915 is overwhelmingly dominated by 4C +39.23A. It shows significant variability at a 6.7$σ$ confidence level and the average $γ$-ray flux in the 0.1--300 GeV energy band is $(1.60\pm 0.15)\times10^{-8}$ ph cm$^{-2}$ s$^{-1}$ with a power-law photon spectral index of $2.48\pm0.05$. During MJD 57500--58500, 4FGL J0824.9+3915 is in a low state with a steady $γ$-ray flux. Analyzed the Fermi/LAT observation data in this time interval, it is found that the TS values of the $γ$-ray emission from 4C +39.23A and 4C +39.23B are $\sim5$ and $\sim 31$, respectively, indicating that the $γ$-ray emission in this time interval is dominated by the CSS 4C +39.23B. The derived average flux in this time interval for 4C +39.23B is $(9.40\pm4.10)\times 10^{-9}$ ph cm $^{-2}$ s$^{-1}$ with $Γ_γ=2.45\pm0.17$. Attributing the spectral energy distribution (SED) of 4C +39.23B to the radiations from its core and extended region, we show that the SED can be represented with a two-zone leptonic model. Its $γ$-ray emission is contributed by the core region. The derived magnetic field strength and Doppler boosting factor of the core are 0.13 G and 6.5. Comparing 4C +39.23B with other $γ$-emitting CSSs and compact symmetric objects (CSOs) in the $Γ_γ-L_γ$ plane, it resembles CSSs.