Comprehensive models of novae at metallicity Z = 0.02 and Z = 10−4

Author:

Chen Hai-Liang1234,Woods T E5,Yungelson L R6,Piersanti Luciano78ORCID,Gilfanov M2910,Han Zhanwen134ORCID

Affiliation:

1. Yunnan Observatories, Chinese Academy of Sciences, Kunming 650011, China

2. Max Planck Institute for Astrophysics, Karl-Schwarzschild-Str 1, Garching b. München D-85741, Germany

3. Key Laboratory for the Structure and Evolution of Celestial Objects, Chinese Academy of Sciences, Kunming 650011, China

4. Center for Astronomical Mega-Science, Chinese Academy of Science, Beijing 100012, China

5. Institute of Gravitational Wave Astronomy and School of Physics and Astronomy, University of Birmingham, Edgbaston, Birmingham B15 2TT, UK

6. Institute of Astronomy, RAS, 48 Pyatnitskaya Str, 119017 Moscow, Russia

7. INAF – Osservatorio Astronomico d’Abruzzo, via Mentore Maggini, snc, I-64100 Teramo, Italy

8. INFN – Sezione di Perugia, via A. Pascoli, I-06123 Perugia, Italy

9. Space Research Institute of Russian Academy of Sciences, Profsoyuznaya 84/32, 117997 Moscow, Russia

10. Kazan Federal University, Kremlevskaya Str 18, 420008 Kazan, Russia

Abstract

ABSTRACT Novae are the observational manifestations of thermonuclear runaways on the surface of accreting white dwarfs (WDs). Although novae are an ubiquitous phenomenon, their properties at low metallicity are not well understood. Using the publicly-available stellar evolution code Modules for Experiments in Stellar Astrophysics (mesa), we model the evolution of accreting carbon–oxygen WDs and consider models that accrete matter with metallicity Z = 0.02 or 10−4. We consider both models without mixing and with matter enriched by CO-elements assuming that mixing occurs in the process of accretion (with mixing fraction 0.25). We present and contrast ignition mass, ejected mass, recurrence period, and maximum luminosity of novae for different WD masses and accretion rates for these metallicities and mixing cases. We find that models with Z  = 0.02 have ignition masses and recurrence periods smaller than models with low Z, while the ejected mass and maximum luminosity are larger. Retention efficiency during novae outbursts decreases with increasing metallicity. In our implementation, inclusion of mixing at the H/He interface reduces accreted mass, ejected mass, and recurrence period as compared to the no-mixing case, while the maximum luminosity becomes larger. Retention efficiency is significantly reduced, becoming negative in most of our models. For ease of use, we provide a tabular summary of our results.

Funder

National Natural Science Foundation of China

Youth Innovation Promotion Association of the Chinese Academy of Sciences

Kazan Federal University

Russian Government Program of Competitive Growth

Yunnan Observatories

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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