The VLA-COSMOS 3 GHz Large Project: Average radio spectral energy distribution of highly star-forming galaxies

The VLA-COSMOS 3 GHz Large Project: Average radio spectral energy distribution of highly star-forming galaxies
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VLA-COSMOS 3 GHz 大型项目:高度恒星形成星系的平均射电频谱能量分布

DOI:
10.1051/0004-6361/201834002
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发表时间:
2019
影响因子:
6.5
通讯作者:
Delhaize
Delhaize
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
Tisanić;Smolčić;Delhaize

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我们构造了高恒星形成星系(HSFGs)的平均射电光谱能量分布(SED)。 红外线和无线电的亮度是由一个紧密的相关性,这是由所谓的q参数定义。这种红外-射电相关性为使用射电光度作为恒星形成示踪剂提供了基础。最近的堆积和生存分析研究发现,q随着红移的增加而减小。有人指出,红移趋势的一个可能原因可能是通过恒星形成星系(SFG)SED的单一幂律假设来计算静止坐标系射电光度。为了测试这一点,我们限制了一个样本的HSFG的无线电SED的形状。为了实现广泛的休息帧频率范围,我们结合了以前发表的超大阵列观测的COSMOS领域在1.4 GHz和3 GHz的未发表的巨型米波射电望远镜(GMRT)观测在325 MHz和610 MHz的生存分析占非检测GMRT地图。    我们选择了一个宽红移范围内的HSFG样本(z∈ [0.3,4],SFR ≥ 100 M yr−1),并构建了平均射电SED。      通过拟合破幂律,我们发现在4.3GHz的静止帧频率以下,谱指数从α1= 0.42 ± 0.06变化到α2= 0.94 ± 0.06。        我们的结果与之前对HSFG(SFR> 10 M μ r −1)的低红移研究一致,这些研究表明HSFG的SED不同于正常SFG(SFR <10 M μ r −1)的SED。      差异主要是在10 GHz左右的陡峭频谱中,这可能表明热自由-自由发射的比例较小。 最后,我们还讨论了应用这种打破幂律SED代替一个简单的幂律inK-校正的HSFG和一个典型的无线电SED从文献中得出的正常SFG的影响。我们发现,无线电SED的形状是不太可能的根本原因theq− z趋势的SFG。
We construct the average radio spectral energy distribution (SED) of highly star-forming galaxies (HSFGs) up toz∼ 4. Infrared and radio luminosities are bound by a tight correlation that is defined by the so-calledqparameter. This infrared–radio correlation provides the basis for the use of radio luminosity as a star-formation tracer. Recent stacking and survival analysis studies findqto be decreasing with increasing redshift. It was pointed out that a possible cause of the redshift trend could be the computation of rest-frame radio luminosity via a single power-law assumption of the star-forming galaxies’ (SFGs) SED. To test this, we constrained the shape of the radio SED of a sample of HSFGs. To achieve a broad rest-frame frequency range, we combined previously published Very Large Array observations of the COSMOS field at 1.4 GHz and 3 GHz with unpublished Giant Meterwave Radio Telescope (GMRT) observations at 325 MHz and 610 MHz by employing survival analysis to account for non-detections in the GMRT maps. We selected a sample of HSFGs in a broad redshift range (z∈ [0.3, 4],  SFR ≥ 100M⊙yr−1) and constructed the average radio SED. By fitting a broken power-law, we find that the spectral index changes fromα1= 0.42 ± 0.06 below a rest-frame frequency of 4.3 GHz toα2= 0.94 ± 0.06 above 4.3 GHz. Our results are in line with previous low-redshift studies of HSFGs ( SFR >  10M⊙yr−1) that show the SED of HSFGs to differ from the SED found for normal SFGs ( SFR <  10M⊙yr−1). The difference is mainly in a steeper spectrum around 10 GHz, which could indicate a smaller fraction of thermal free–free emission. Finally, we also discuss the impact of applying this broken power-law SED in place of a simple power-law inK-corrections of HSFGs and a typical radio SED for normal SFGs drawn from the literature. We find that the shape of the radio SED is unlikely to be the root cause of theq−ztrend in SFGs.
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