Unveiling the white dwarf in J191213.72 − 441045.1 through ultraviolet observations

Author:

Pelisoli Ingrid1ORCID,Sahu Snehalata1ORCID,Lyutikov Maxim2ORCID,Barkov Maxim3ORCID,Gänsicke Boris T1ORCID,Brink Jaco45,Buckley David A H456ORCID,Potter Stephen B47ORCID,Schwope Axel8,Ramírez S H1ORCID

Affiliation:

1. Department of Physics, University of Warwick , Gibbet Hill Road, Coventry, CV4 7AL , UK

2. Department of Physics and Astronomy, Purdue University , 525 Northwestern Avenue, West Lafayette,47907 IN , USA

3. Institute of Astronomy, Russian Academy of Sciences , 119017 Moscow , Russia

4. South African Astronomical Observatory , PO Box 9, Observatory, 7935 Cape Town , South Africa

5. Department of Astronomy, University of Cape Town , Private Bag X3, 7701 Rondebosch , South Africa

6. Department of Physics, University of the Free State , PO Box 339,9300 Bloemfontein , South Africa

7. Department of Physics, University of Johannesburg , PO Box 524, 2006 Auckland Park , South Africa

8. Leibniz-Institut für Astrophysik Potsdam (AIP) , An der Sternwarte 16, D-14482 Potsdam , Germany

Abstract

ABSTRACT J191213.72 − 441045.1 is a binary system composed of a white dwarf and an M-dwarf in a 4.03-h orbit. It shows emission in radio, optical, and X-ray, all modulated at the white dwarf spin period of 5.3 min, as well as various orbital sideband frequencies. Like in the prototype of the class of radio-pulsing white dwarfs, AR Scorpii, the observed pulsed emission seems to be driven by the binary interaction. In this work, we present an analysis of far-ultraviolet spectra obtained with the Cosmic Origins Spectrograph at the Hubble Space Telescope, in which we directly detect the white dwarf in J191213.72 − 441045.1. We find that the white dwarf has a temperature of Teff = 11485 ± 90 K and mass of 0.59 ± 0.05 M⊙. We place a tentative upper limit on the magnetic field of ≈50 MG. If the white dwarf is in thermal equilibrium, its physical parameters would imply that crystallization has not started in the core of the white dwarf. Alternatively, the effective temperature could have been affected by compressional heating, indicating a past phase of accretion. The relatively low upper limit to the magnetic field and potential lack of crystallization that could generate a strong field pose challenges to pulsar-like models for the system and give preference to propeller models with a low magnetic field. We also develop a geometric model of the binary interaction which explains many salient features of the system.

Funder

Deutsche Forschungsgemeinschaft

NASA

ESA

European Research Council

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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