射电测量中的恒星形成:将90 GHz数据添加到附近星系恒星形成区域的3-33 GHz观测中

Anna Dignan, Eric J. Murphy, Brian Mason, Cosima Eibensteiner, Brandon S. Hensley, Eric F. Jiménez-Andrade, Sean T. Linden, Simon R. Dicker, Dillon Z. Dong, Emmanuel Momjian, Charles E. Romero, Eva Schinnerer and Jean L. Turner
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摘要

作为射电巡天中恒星形成的一部分,我们展示了用Robert C. Byrd Green Bank望远镜上的MUSTANG-2观测到的30个邻近星系的119个恒星形成区域的90 GHz连续成像。90 GHz数据与之前由Karl G. Jansky甚大阵列采集的3、15和33 GHz数据相结合,将约0.8 kpc尺度上的无线电频谱分解为同步加速器、自由-自由和热尘埃发射成分。这是通过三种情况完成的:(i)幂律拟合从3到33 GHz, (ii)马尔可夫链蒙特卡罗(MCMC)拟合从3到90 GHz,含热粉尘成分,(iii) MCMC拟合从3到33 GHz,不含热粉尘成分。对于这些情况,我们发现33 GHz的中位热(自由-自由)发射分数为(i) 88%±2%,散射为17%;(ii) 76%±3%,散射为25%;(iii) 84%±2%,散射为18%。由此我们得出结论,平均而言,自由-自由发射,而不是热尘埃,仍然是33 GHz的主要发射成分。虽然情景(ii)产生的热分数比情景(iii)大约10%,但在移除活动星系核后,这一差异减小至约5%。因此,在没有90 GHz光谱分解数据的情况下,用33 GHz热分量测量的恒星形成率只有轻微的高偏差。此外,从3到33 GHz的数据的幂律拟合仍然提供了33 GHz的自由-自由发射的可靠估计。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Star Formation in Radio Survey: Adding 90 GHz Data to 3–33 GHz Observations of Star-forming Regions in Nearby Galaxies
We present 90 GHz continuum imaging of 119 star-forming regions in 30 nearby galaxies observed with MUSTANG-2 on the Robert C. Byrd Green Bank Telescope as part of the Star Formation in Radio Survey. The 90 GHz data were combined with 3, 15, and 33 GHz data taken previously by the Karl G. Jansky Very Large Array to decompose radio spectra on ≈0.8 kpc scales into their synchrotron, free–free, and thermal dust emission components. This was done using three scenarios: (i) a power-law fit from 3 to 33 GHz, (ii) Markov Chain Monte Carlo (MCMC) fitting from 3 to 90 GHz with a thermal dust component, and (iii) MCMC fitting from 3 to 33 GHz without a thermal dust component. For these cases, we find a median thermal (free–free) emission fraction at 33 GHz of (i) 88% ± 2% with a scatter of 17%, (ii) 76% ± 3% with a scatter of 25%, and (iii) 84% ± 2% with a scatter of 18%. From this we conclude that, on average, free–free emission, not thermal dust, remains the dominant emission component at 33 GHz. While scenario (ii) yields a thermal fraction that is ≈10% larger than scenario (iii), this difference decreases to ≈5% after active galactic nuclei are removed. Consequently, star formation rates measured with thermal fractions at 33 GHz are only mildly biased high without 90 GHz data for the spectral decomposition. Furthermore, a power-law fit of data from 3 to 33 GHz still provides a reliable estimate of the free–free emission at 33 GHz.
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