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Measurement of the extragalactic background light at 8600 Å using dark cloud shadow and the Ca II-triplet lines




TekijätHaikala, L. K.; Mattila, K.; Väisänen, P.

KustantajaEDP Sciences

Julkaisuvuosi2026

Lehti: Astronomy and Astrophysics

Artikkelin numeroA358

Vuosikerta706

ISSN0004-6361

eISSN1432-0746

DOIhttps://doi.org/10.1051/0004-6361/202557566

Julkaisun avoimuus kirjaamishetkelläAvoimesti saatavilla

Julkaisukanavan avoimuus Kokonaan avoin julkaisukanava

Verkko-osoitehttps://doi.org/10.1051/0004-6361/202557566

Rinnakkaistallenteen osoitehttps://research.utu.fi/converis/portal/detail/Publication/515779838

Rinnakkaistallenteen lisenssiCC BY

Rinnakkaistallennetun julkaisun versioKustantajan versio


Tiivistelmä

We present the results of a measurement of the near-infrared extragalactic background light (EBL). The surface brightness towards the opaque intermediate-latitude globule DC303.8-14.2 was obtained using ESO VLT/FORS spectrophotometry. Long-slit spectra covering the opaque core and the almost unobscured area north of the cloud were measured using the nodding-along-the-slit measuring technique, thus providing a differential spectrum opaque core – transparent area. It is free of most of the foreground components, also excluding most of the airglow time variations. The scattered integrated starlight (ISL) from the dark core itself is the only remaining major foreground component when extracting the EBL from the differential spectrum. The scattered starlight spectrum in the wavelength domain 8450–8700 Å is dominated by the strong Ca II triplet Fraunhofer lines at λ 8498, 8542, 8664 Å, whereas the integrated light of galaxies and other contributors to the EBL intensity produce a smooth spectrum without these lines. We used the GAIA RVS spectral database to construct a template for the scattered ISL spectrum; another template was obtained by using the globule’s semi-transparent bright rim. The resulting EBL intensity as derived from the λ 8542 Å line is IEBL = 1.62 ± 0.76(σstat) 10−9 erg cm−2 s−1 Å−1 sterad−1 or 13.8 ± 6.5(σstat) nW m−2 sr−1; this represents a tentative detection at 2.1σ level; the scaling uncertainty is ±10%.


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