Variability of the near-infrared extinction curve towards the Galactic centre

Context. Due to the extreme extinction towards the Galactic centre (AV ∼ 30 mag), its stellar population is mainly studied in the near-infrared (NIR) regime. Therefore, a proper analysis of the NIR extinction curve is necessary to fully characterise the stellar structure and population of the inner...

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Detalhes bibliográficos
Autores: Nogueras Lara, F., Schödel, R., Najarro, F., Gallego Calvente, A. T., Gallego Cano, E., Shahzamanian, B., Neumayer, N.
Tipo de documento: artigo
Estado:Versão publicada
Data de publicação:2019
País:España
Recursos:Instituto Nacional de Técnica Aeroespacial (INTA)
Repositório:DIGITAL.INTA Repositorio Digital del Instituto Nacional de Técnica Aeroespacial
OAI Identifier:oai:digital.inta.es:20.500.12666/349
Acesso em linha:https://www.aanda.org/articles/aa/full_html/2019/10/aa36322-19/aa36322-19.html
http://hdl.handle.net/20.500.12666/349
Access Level:Acceso aberto
Palavra-chave:Galaxy: nucleus
Dust
Extinction
Galaxy: center
Stars: horizontal-branch
Descrição
Resumo:Context. Due to the extreme extinction towards the Galactic centre (AV ∼ 30 mag), its stellar population is mainly studied in the near-infrared (NIR) regime. Therefore, a proper analysis of the NIR extinction curve is necessary to fully characterise the stellar structure and population of the inner part of the galaxy. Aims. We studied the dependence of the extinction index (αλ) in the NIR on the line of sight, wavelength, and extinction. Methods. We used the GALACTICNUCLEUS imaging survey, a high angular resolution catalogue (0.2″) for the inner part of the Galaxy in JHKs, and studied the spatial variation in the extinction index. We also applied two independent methods based on red clump stars to compute the extinction index between different bands and its variation with wavelength. Results. We did not detect any significant line-of-sight or extinction variation in α within the studied region in the nuclear stellar disc. The extinction index between JH and HKs differs by 0.19 ± 0.05. We obtained mean values for the extinction indices αJH = 2.43 ± 0.03 and αHKs = 2.23 ± 0.03. The dependence of the extinction index on the wavelength could explain the differences obtained for αλ in the literature since it was assumed constant for the NIR regime.