dorsal/arxiv
View SchemaCosmoglobe DR2. V. Spatial correlations between thermal dust and ionized carbon emission in Planck HFI and COBE-DIRBE
| Authors | E. Gjerløw, R. M. Sullivan, R. Aurvik, A. Basyrov, L. A. Bianchi, A. Bonato, M. Brilenkov, H. K. Eriksen, U. Fuskeland, M. Galloway, K. A. Glasscock, L. T. Hergt, D. Herman, J. G. S. Lunde, M. San, A. I. Silva Martins, D. Sponseller, N. -O. Stutzer, H. Thommesen, V. Vikenes, D. J. Watts, I. K. Wehus, L. Zapelli |
|---|---|
| Categories | |
| ArXiv ID | 2601.07818vv1 |
| URL | https://arxiv.org/abs/2601.07818 |
| License | http://creativecommons.org/licenses/by/4.0/ |
Abstract
We fit five tracers of thermal dust emission to ten Planck HFI and COBE-DIRBE frequency maps between 353 GHz and 25 THz, aiming to map the relative importance of each physical host environment as a function of frequency and position on the sky. Four of these correspond to classic thermal dust tracers, namely H i (HI4PI), CO (Dame et al. 2001a), H{\alpha} (WHAM, Haffner et al. (2003a, 2016)), and dust extinction (Gaia; Edenhofer et al. 2024), while the fifth is ionized carbon (C ii) emission as observed by COBE- FIRAS. We jointly fit these five templates to each frequency channel through standard multi-variate linear regression. At frequencies higher than 1 THz, we find that the dominant tracer is in fact C ii, and above 10 THz this component accounts for almost the entire fitted signal; at frequencies below 1 THz, its importance is second only to H i. We further find that all five components are well described by a modified blackbody spectral energy density (SED) up to some component-dependent maximum frequency ranging between 1 and 5 THz. In this interpretation, the C ii-correlated component is the hottest among all five, with an effective temperature of about 25 K. The H{\alpha} component has a temperature of 18 K, and, unlike the other four, is observed in absorption rather than emission. Despite the simplicity of this model, which relies only on external templates coupled to spatially isotropic SEDs, we find that it captures 98 % of the full signal root mean squared (RMS) below 1 THz. This high efficiency suggests that spatial variations in the thermal dust SED, as for instance reported by Planck and other experiments, may be more economically modelled on large angular scales in terms of a spatial mixing of individually isotropic physical components.
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"abstract": "We fit five tracers of thermal dust emission to ten Planck HFI and COBE-DIRBE frequency maps between 353 GHz and 25 THz, aiming to map the relative importance of each physical host environment as a function of frequency and position on the sky. Four of these correspond to classic thermal dust tracers, namely H i (HI4PI), CO (Dame et al. 2001a), H{\\alpha} (WHAM, Haffner et al. (2003a, 2016)), and dust extinction (Gaia; Edenhofer et al. 2024), while the fifth is ionized carbon (C ii) emission as observed by COBE- FIRAS. We jointly fit these five templates to each frequency channel through standard multi-variate linear regression. At frequencies higher than 1 THz, we find that the dominant tracer is in fact C ii, and above 10 THz this component accounts for almost the entire fitted signal; at frequencies below 1 THz, its importance is second only to H i. We further find that all five components are well described by a modified blackbody spectral energy density (SED) up to some component-dependent maximum frequency ranging between 1 and 5 THz. In this interpretation, the C ii-correlated component is the hottest among all five, with an effective temperature of about 25 K. The H{\\alpha} component has a temperature of 18 K, and, unlike the other four, is observed in absorption rather than emission. Despite the simplicity of this model, which relies only on external templates coupled to spatially isotropic SEDs, we find that it captures 98 % of the full signal root mean squared (RMS) below 1 THz. This high efficiency suggests that spatial variations in the thermal dust SED, as for instance reported by Planck and other experiments, may be more economically modelled on large angular scales in terms of a spatial mixing of individually isotropic physical components.",
"arxiv_id": "2601.07818",
"authors": [
"E. Gjerl\u00f8w",
"R. M. Sullivan",
"R. Aurvik",
"A. Basyrov",
"L. A. Bianchi",
"A. Bonato",
"M. Brilenkov",
"H. K. Eriksen",
"U. Fuskeland",
"M. Galloway",
"K. A. Glasscock",
"L. T. Hergt",
"D. Herman",
"J. G. S. Lunde",
"M. San",
"A. I. Silva Martins",
"D. Sponseller",
"N. -O. Stutzer",
"H. Thommesen",
"V. Vikenes",
"D. J. Watts",
"I. K. Wehus",
"L. Zapelli"
],
"categories": [
"astro-ph.CO",
"astro-ph.GA"
],
"license": "http://creativecommons.org/licenses/by/4.0/",
"title": "Cosmoglobe DR2. V. Spatial correlations between thermal dust and ionized carbon emission in Planck HFI and COBE-DIRBE",
"url": "https://arxiv.org/abs/2601.07818",
"version": "v1"
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