论文标题

GMRT在323 MHz的Radio-Loud类星体上观察到$ z> 5 $

Observations by GMRT at 323 MHz of radio-loud quasars at $z>5$

论文作者

Shao, Yali, Wagg, Jeff, Wang, Ran, Carilli, Chris L., Riechers, Dominik A., Intema, Huib T., Weiss, Axel, Menten, Karl M.

论文摘要

我们提出了巨大的Metrewave射电望远镜(GMRT)323 MHz无线电连续观测,该观测值是$ Z> 5 $,对13个无线电大型类星体进行观察,从这些物体中抽样低频同步器发射。在成功观察到的12个目标中,我们检测到10美元以上的4σ$显着性,而2个未被发现。所有检测到的来源都作为点源。结合文献的先前无线电连续探测,9个类星体在整个无线电范围内具有幂律光谱分布。对于某些磁通量密度的频率下降,而其他磁通密度则增加。这些来源中的两个似乎具有光谱转移。对于类似幂律的来源,幂律指数的正范围在0.18至0.67之间,负值在$ -0.90 $和$ -0.27 $之间。对于失误来源,电台在$ \ sim1 $和$ \ sim10 $ ghz左右的峰值上的峰值峰值,光学薄索引为$ -0.58 $和$ -0.90 $,光学较厚的指数为0.50和1.20。 SDSS J114657.59+403708.6 $ z = 5.01 $的磁场和频谱年龄分析可能表明,转移不是由同步体自我吸收,而是由核区域的高密度培养基通过高密度培养基的免费免费吸收。另外,明显的营业额可能是源可变性的伪像。最后,我们为我们的样本计算了无线电响度$ r_ {2500 \ rm \,Å} $,该样品的范围从12 $^{+13} _ { - 13} $到4982 $^{+279} _ { - 254} $。

We present Giant Metrewave Radio Telescope (GMRT) 323 MHz radio continuum observations toward 13 radio-loud quasars at $z>5$, sampling the low-frequency synchrotron emission from these objects. Among the 12 targets successfully observed, we detected 10 above $4σ$ significance, while 2 remain undetected. All of the detected sources appear as point sources. Combined with previous radio continuum detections from the literature, 9 quasars have power-law spectral energy distributions throughout the radio range; for some the flux density drops with increasing frequency while it increases for others. Two of these sources appear to have spectral turnover. For the power-law-like sources, the power-law indices have a positive range between 0.18 and 0.67 and a negative values between $-0.90$ and $-0.27$. For the turnover sources, the radio peaks around $\sim1$ and $\sim10$ GHz in the rest frame, the optically thin indices are $-0.58$ and $-0.90$, and the optically thick indices are 0.50 and 1.20. A magnetic field and spectral age analysis of SDSS J114657.59+403708.6 at $z=5.01$ may indicate that the turnover is not caused by synchrotron self-absorption, but rather by free-free absorption by the high-density medium in the nuclear region. Alternatively, the apparent turnover may be an artifact of source variability. Finally, we calculated the radio loudness $R_{2500\rm\, Å}$ for our sample, which spans a very wide range from 12$^{+13}_{-13}$ to 4982$^{+279}_{-254}$.

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