Revisiting the classics: On the evolutionary origin of the "Fe II" and "He/N" spectral classes of novae

dc.contributor.authorAydi, E.
dc.contributor.authorChomiuk, L.
dc.contributor.authorStrader, J.
dc.contributor.authorSokolovsky, K. V.
dc.contributor.authorMukai, Koji
dc.contributor.authoret al
dc.date.accessioned2023-10-10T15:55:36Z
dc.date.available2023-10-10T15:55:36Z
dc.date.issued2023-09-13
dc.descriptionAuthors: E. Aydi, L. Chomiuk, J. Strader, K. V. Sokolovsky, R. E. Williams, D. A. H. Buckley, A. Ederoclite, L. Izzo, R. Kyer, J. D. Linford, A. Kniazev, B. D. Metzger, J. Mikolajewska, P. Molaro, I. Mollina, K. Mukai, U. Munari, M. Orio, T. Panurach, B. J. Shappee, K. J. Shen, J. L. Sokoloski, R. Urquhart, F. M. Walteren_US
dc.description.abstractThe optical spectra of novae are characterized by emission lines from the hydrogen Balmer series and either Fe II or He/N, leading to their traditional classification into two spectral classes: "Fe II" and "He/N". For decades, the origins of these spectral features were discussed in the literature in the contexts of different bodies of gas or changes in the opacity of the ejecta, particularly associated with studies by R. E. Williams and S. N. Shore. Here, we revisit these major studies with dedicated, modern data sets, covering the evolution of several novae from early rise to peak all the way to the nebular phase. Our data confirm previous suggestions in the literature that the "Fe II" and "He/N" spectral classes are phases in the spectroscopic evolution of novae driven primarily by changes in the opacity, ionization, and density of the ejecta, and most if not all novae go through at least three spectroscopic phases as their eruptions evolve: an early He/N (phase 1; observed during the early rise to visible peak and characterized by P Cygni lines of He I, N II, and N III), then an Fe II (phase 2; observed near visible peak and characterized by P Cygni lines of Fe II and O I), and then a later He/N (phase 3; observed during the decline and characterized by emission lines of He I. He II, N II, and N III), before entering the nebular phase. This spectral evolution seems to be ubiquitous across novae, regardless of their speed class; however the duration of each of these phase differs based on the speed class of the nova.en_US
dc.description.sponsorshipE.A. acknowledges support by NASA through the NASA Hubble Fellowship grant HST-HF2-51501.001-A awarded by the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA, under contract NAS5-26555. LC acknowledges NSF awards AST-1751874 and AST-2107070 and a Cottrell fellowship of the Research Corporation. JS was supported by the Packard Foundation. DAHB gratefully acknowledges the receipt of research grants from the National Research Foundation (NRF) of South Africa. AK acknowledges the Ministry of Science and Higher Education of the Russian Federation grant 075-15-2022-262 (13.MNPMU.21.0003). BDM is supported in part by NASA (grants 80NSSC22K0807 and 80NSSC22K1573). JM was supported by the National Science Centre, Poland, grant OPUS 2017/27/B/ST9/01940. KJS is supported by NASA through the Astrophysics Theory Program (80NSSC20K0544). A part of this work is based on observations made with the Southern African Large Telescope (SALT), with the Large Science Programme on transients 2021-2-LSP-001 (PI: DAHB). Polish participation in SALT is funded by grant No. MEiN 2021/WK/01. This paper was partially based on observations obtained at the Southern Astrophysical Research (SOAR) telescope, which is a joint project of the Minist´erio da Ciˆencia, Tecnologia e Inova¸c˜oes (MCTI/LNA) do Brasil, the US National Science Foundation’s NOIRLab, the University of North Carolina at Chapel Hill (UNC), and Michigan State University (MSU). Analysis made significant use of python 3.7.4, and the associated packages numpy, matplotlib, seaborn, scipy. Data reduction made significant use of MIDAS FEROS (Stahl et al. 1999), echelle (Ballester 1992), PySALT (Crawford et al. 2010), and IRAF (Tody 1986, 1993).en_US
dc.description.urihttps://arxiv.org/abs/2309.07097en_US
dc.format.extent21 pagesen_US
dc.genrejournal articlesen_US
dc.genrepreprintsen_US
dc.identifierdoi:10.13016/m2r6nf-e40d
dc.identifier.urihttps://doi.org/10.48550/arXiv.2309.07097
dc.identifier.urihttp://hdl.handle.net/11603/30037
dc.language.isoen_USen_US
dc.relation.isAvailableAtThe University of Maryland, Baltimore County (UMBC)
dc.relation.ispartofUMBC Center for Space Sciences and Technology
dc.relation.ispartofUMBC Faculty Collection
dc.rightsThis item is likely protected under Title 17 of the U.S. Copyright Law. Unless on a Creative Commons license, for uses protected by Copyright Law, contact the copyright holder or the author.en_US
dc.rightsAttribution-NonCommercial-NoDerivs 4.0 International*
dc.rights.urihttps://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.titleRevisiting the classics: On the evolutionary origin of the "Fe II" and "He/N" spectral classes of novaeen_US
dc.typeTexten_US
dcterms.creatorhttps://orcid.org/0000-0002-8286-8094en_US

Files

Original bundle

Now showing 1 - 1 of 1
Loading...
Thumbnail Image
Name:
2309.07097.pdf
Size:
3.76 MB
Format:
Adobe Portable Document Format
Description:

License bundle

Now showing 1 - 1 of 1
Loading...
Thumbnail Image
Name:
license.txt
Size:
2.56 KB
Format:
Item-specific license agreed upon to submission
Description: