Continuous evolution of the polarization properties in the transient X-ray pulsar RX J0440.9+4431/LS V +44 17

dc.contributor.authorZhao, Q. C.
dc.contributor.authorTao, L.
dc.contributor.authorTsygankov, S. S.
dc.contributor.authorMushtukov, A. A.
dc.contributor.authorFeng, H.
dc.contributor.authorGe, M. Y.
dc.contributor.authorLi, H. C.
dc.contributor.authorZhang, S. N.
dc.contributor.authorZhang, L.
dc.contributor.organizationfi=Tuorlan observatorio|en=Tuorla Observatory|
dc.contributor.organization-code1.2.246.10.2458963.20.90670098848
dc.converis.publication-id485102688
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/485102688
dc.date.accessioned2025-08-27T21:35:56Z
dc.date.available2025-08-27T21:35:56Z
dc.description.abstractWe present a detailed time-resolved and phase-resolved polarimetric analysis of the transient X-ray pulsar RX J0440.9+4431/LS V +44 17, using data from the Imaging X-ray Polarimetry Explorer (IXPE) during the 2023 giant outburst. We conducted a time-resolved analysis by dividing the data into several intervals for each observation. This analysis reveals a continuous rotation of the phase-averaged polarization angle (PA) across the observations performed during the supercritical and subcritical regimes. To investigate the origin of the PA rotation, we performed a pulse phase-resolved polarimetric analysis over four time intervals, each spanning approximately three days. Applying the rotating vector model (RVM), the geometric parameters of the system were determined for each interval. Despite the short time gap of just similar to 20 days, we observed significant variation in the RVM parameters between the first interval and the subsequent three, indicating the presence of an additional polarized component alongside the RVM component. Using a two-polarized component model with the assumption that this additional component remains constant across pulse phases, we calculated the phase-averaged PA and polarized flux of both the variable and constant components. The phase-averaged PA of each component remained relatively stable over time, but the polarized flux of the constant component decreased, while that of the variable component increased. The observed rotation of the PA is attributed to the gradual shift in the polarized flux ratio between the two components and is not directly related to the different accretion regimes.
dc.identifier.eissn1432-0746
dc.identifier.jour-issn0004-6361
dc.identifier.olddbid200702
dc.identifier.oldhandle10024/183729
dc.identifier.urihttps://www.utupub.fi/handle/11111/46759
dc.identifier.urlhttps://doi.org/10.1051/0004-6361/202452872
dc.identifier.urnURN:NBN:fi-fe2025082785095
dc.language.isoen
dc.okm.affiliatedauthorTsygankov, Sergey
dc.okm.discipline115 Astronomy and space scienceen_GB
dc.okm.discipline115 Avaruustieteet ja tähtitiedefi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherEDP Sciences
dc.publisher.countryFranceen_GB
dc.publisher.countryRanskafi_FI
dc.publisher.country-codeFR
dc.publisher.placeLES ULIS CEDEX A
dc.relation.articlenumberA241
dc.relation.doi10.1051/0004-6361/202452872
dc.relation.ispartofjournalAstronomy and Astrophysics
dc.relation.volume693
dc.source.identifierhttps://www.utupub.fi/handle/10024/183729
dc.titleContinuous evolution of the polarization properties in the transient X-ray pulsar RX J0440.9+4431/LS V +44 17
dc.year.issued2025

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