J 2020

Structure of accretion flows in the nova-like cataclysmic variable RW Tri

SUBEBEKOVA, G., S. ZHARIKOV, G. TOVMASSIAN, V. NEUSTROEV, M. WOLF et. al.

Basic information

Original name

Structure of accretion flows in the nova-like cataclysmic variable RW Tri

Authors

SUBEBEKOVA, G., S. ZHARIKOV, G. TOVMASSIAN, V. NEUSTROEV, M. WOLF, M-S HERNANDEZ, Hana KUČÁKOVÁ (203 Czech Republic, belonging to the institution) and S. KHOKHLOV

Edition

Monthly Notices of the Royal Astronomical Society, 2020, 0035-8711

Other information

Language

English

Type of outcome

Článek v odborném periodiku

Field of Study

10308 Astronomy

Country of publisher

United Kingdom of Great Britain and Northern Ireland

Confidentiality degree

není předmětem státního či obchodního tajemství

References:

RIV identification code

RIV/47813059:19630/20:A0000069

Organization unit

Institute of physics in Opava

UT WoS

000574924500014

Keywords in English

binaries: spectroscopic; stars: individual: RW Tri; novae; cataclysmic variables

Tags

Tags

International impact, Reviewed
Změněno: 31/3/2022 10:32, Mgr. Pavlína Jalůvková

Abstract

V originále

We obtained photometric observations of the nova-like (NL) cataclysmic variable RW Tri and gathered all available AAVSO and other data from the literature. We determined the system parameters and found their uncertainties using the code developed by us to model the light curves of binary systems. New time-resolved optical spectroscopic observations of RW Tri were also obtained to study the properties of emission features produced by the system. The usual interpretation of the single-peaked emission lines in NL systems is related to the bi-conical wind from the accretion disc's inner part. However, we found that the Ha emission profile is comprised of two components with different widths. We argue that the narrow component originates from the irradiated surface of the secondary, while the broader component's source is an extended, low-velocity region in the outskirts of the accretion disc, located opposite to the collision point of the accretion stream and the disc. It appears to be a common feature for long-period NL systems - a point we discuss.