利用 JWST 近红外成像仪对 z=0.7-2 波段的尘埃和多环芳烃进行新的普查

I. Shivaei, S. Alberts, M. Florian, G. Rieke, S. Wuyts, Sarah Bodansky, J. Andrew Bunker, J. Alex Cameron, M. Curti, F. d’Eugenio, U. Dudzevičiūtė, Zhiyuan Ji, D. Benjamin Johnson, I. Kramarenko, J. Lyu, J. Matthee, Jane Morrison, R. Naidu, G. Pablo P'erez-Gonz'alez, Naveen A. Reddy, B. Robertson, Yang Sun, S. Tacchella, K. Whitaker, C. Christina Williams, N.A. Christopher Willmer, J. Witstok, M. Xiao, Yongda Zhu
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摘要

本文利用詹姆斯-韦伯太空望远镜(JWST)的中红外仪器(MIRI),将对尘埃和多环芳烃(PAH)发射的观测研究扩展到本地宇宙以外的新质量和恒星形成率(SFR)参数空间。结合多个中红外波段的全采样光谱能量分布(SED)和 MIRI 前所未有的灵敏度,我们可以研究典型主序星系中从 $z=0.7$ 到 $z=2$ 的尘埃遮蔽和多环芳烃行为。我们的重点是在宇宙正午(宇宙中恒星形成活动的高峰期)之前和期间制约多环芳香烃强度和尘埃遮蔽光度分数的演变。我们发现 PAHs 中的尘埃比例(PAH 分数 qpah)与恒星质量之间有很强的相关性。此外,对qpah进行了可靠测量的子样本($N=216$)显示,qpah与气相金属性之间的关系与在$z时的关系类似,表明了一种普遍关系:在金属性为$Z odot$时,qpah是恒定的($ 3.4$),平均下降到$5 Msun时,超过一半的发射光度被遮挡,而存在一个不可忽略的低质量星系群,其遮挡率为$>50$。在质量固定的情况下,遮蔽率与SFR表面密度相关。这是因为在恒星形成区比较紧凑的星系中,尘埃覆盖率较高。同样,在一定质量或紫外连续波斜率(β)下,IRX(红外-紫外光度)高的星系往往具有更高的Ssfr和更浅的衰减曲线,这是因为它们的有效尘埃光学深度更高,恒星形成区更紧凑。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A new census of dust and polycyclic aromatic hydrocarbons at z=0.7-2 with JWST MIRI
This paper utilises the James Webb Space Telescope (JWST) Mid-Infrared Instrument (MIRI) to extend the observational studies of dust and polycyclic aromatic hydrocarbon (PAH) emission to a new mass and star formation rate (SFR) parameter space beyond our local Universe. The combination of fully sampled spectral energy distributions (SEDs) with multiple mid-infrared (mid-IR) bands and the unprecedented sensitivity of MIRI allows us to investigate dust obscuration and PAH behaviour from $z=0.7$ up to $z=2$ in typical main-sequence galaxies. Our focus is on constraining the evolution of PAH strength and the dust-obscured luminosity fraction before and during cosmic noon, the epoch of peak star formation activity in the Universe. um um um um imaging data, enhancing our understanding of the physical characteristics of dust within these galaxies. We find a strong correlation between the fraction of dust in PAHs (PAH fraction qpah ) with stellar mass. Moreover the sub-sample with robust qpah measurements ($N=216$) shows a similar behaviour between qpah and gas-phase metallicity to that at $z suggesting a universal relation: qpah is constant ($ 3.4$) above a metallicity of $Z odot $ and decreases to $<1$ at metallicities $ odot $. This indicates that metallicity is a good indicator of the interstellar medium properties that affect the balance between the formation and destruction of PAHs. The lack of a redshift evolution from $z 0-2$ also implies that above $Z odot $ the PAH emission effectively traces obscured luminosity and the previous locally calibrated PAH-SFR calibrations remain applicable in this metallicity regime. We observe a strong correlation between the obscured UV luminosity fraction (ratio of obscured to total luminosity) and stellar mass. Above the stellar mass of $M_*>5 Msun on average, more than half of the emitted luminosity is obscured, while there exists a non-negligible population of lower-mass galaxies with $>50$ obscured fractions. At a fixed mass, the obscured fraction correlates with SFR surface density. This is a result of higher dust covering fractions in galaxies with more compact star-forming regions. Similarly, galaxies with high IRX (IR to UV luminosity) at a given mass or UV continuum slope (beta ) tend to have higher Ssfr and shallower attenuation curves, owing to their higher effective dust optical depths and more compact star-forming regions.
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