Detailed Information on Publication Record
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
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.