Emergence hour-by-hour of r-process features in the kilonova AT2017gfo

dc.contributor.authorSneppen, Albert
dc.contributor.authorWatson, Darach
dc.contributor.authorDamgaard, Rasmus
dc.contributor.authorHeintz, Kasper E.
dc.contributor.authorVieira, Nicholas
dc.contributor.authorVäisänen, Petri
dc.contributor.authorMahoro, Antoine
dc.contributor.organizationfi=Suomen ESO-keskus|en=Finnish Centre for Astronomy with ESO|
dc.contributor.organization-code1.2.246.10.2458963.20.54954054844
dc.converis.publication-id459294932
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/459294932
dc.date.accessioned2025-08-27T22:56:55Z
dc.date.available2025-08-27T22:56:55Z
dc.description.abstract<p>The spectral features in the optical/near-infrared counterparts of neutron star mergers (kilonovae, KNe) evolve dramatically on hourly timescales. To examine the spectral evolution, we compiled a temporal series that was complete at all observed epochs from 0.5 to 9.4 days of the best optical/near-infrared (NIR) spectra of the gravitational-wave detected kilonova AT2017gfo. Using our analysis of this spectral series, we show that the emergence times of spectral features place strong constraints on line identifications and ejecta properties, while their subsequent evolution probes the structure of the ejecta. We find that the most prominent spectral feature, the 1 μm P Cygni line, appears suddenly, with the earliest detection at 1.17 days. We find evidence in this earliest feature for the fastest yet discovered kilonova ejecta component at 0.40-0.45c. Across the observed epochs and wavelengths, the velocities of the line-forming regions span nearly an order of magnitude, down to as low as 0.04-0.07c. The time of emergence closely follows the predictions for Sr II because Sr III combines rapidly under local thermal equilibrium (LTE) conditions. The transition time between the doubly and singly ionised states provides the first direct measurement of the ionisation temperature. This temperature is highly consistent with the temperature of the emitted blackbody radiation field at a level of a few percent. Furthermore, we find the KN to be isotropic in temperature, that is, the polar and equatorial ejecta differ by less than a few hundred Kelvin or ≲5%, in the first few days post-merger based on measurements of the reverberation time-delay effect. This suggests that a model with very simple assumptions, with single-temperature LTE conditions, reproduces the early kilonova properties surprisingly well.<br></p>
dc.identifier.eissn1432-0746
dc.identifier.jour-issn0004-6361
dc.identifier.olddbid203092
dc.identifier.oldhandle10024/186119
dc.identifier.urihttps://www.utupub.fi/handle/11111/50699
dc.identifier.urlhttps://doi.org/10.1051/0004-6361/202450317
dc.identifier.urnURN:NBN:fi-fe2025082785961
dc.language.isoen
dc.okm.affiliatedauthorVäisänen, Petri
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.articlenumberA398
dc.relation.doi10.1051/0004-6361/202450317
dc.relation.ispartofjournalAstronomy and Astrophysics
dc.relation.volume690
dc.source.identifierhttps://www.utupub.fi/handle/10024/186119
dc.titleEmergence hour-by-hour of r-process features in the kilonova AT2017gfo
dc.year.issued2024

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