Evidence for asymmetric distribution of circumstellar material around type Ia supernovae
Author
dc.contributor.author
Förster, Francisco
Author
dc.contributor.author
González Gaitán, Santiago
es_CL
Author
dc.contributor.author
Anderson, Joseph
es_CL
Author
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Marchi, Sebastián
es_CL
Author
dc.contributor.author
Gutiérrez, Claudia P.
Author
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Hamuy Wackenhut, Mario
Author
dc.contributor.author
Pignata Libralato, Giuliano
Author
dc.contributor.author
Cartier Ugarte, Regis
Admission date
dc.date.accessioned
2014-01-03T18:10:22Z
Available date
dc.date.available
2014-01-03T18:10:22Z
Publication date
dc.date.issued
2012-08-01
Cita de ítem
dc.identifier.citation
The Astrophysical Journal Letters, 754:L21 (5pp), 2012 August 1
en_US
Identifier
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DOI: 10.1088/2041-8205/754/2/L21
Identifier
dc.identifier.uri
https://repositorio.uchile.cl/handle/2250/125948
Abstract
dc.description.abstract
We study the properties of low-velocity material in the line of sight toward nearby Type Ia supernovae (SNe Ia) that
have measured late phase nebular velocity shifts (vneb), thought to be an environment-independent observable. We
have found that the distribution of equivalent widths of narrow blended Na i D1 and D2 and Ca ii H and K absorption
lines differs significantly between those SNe Ia with negative and positive vneb, with generally stronger absorption
for SNe Ia with vneb 0. A similar result had been found previously for the distribution of colors of SNe Ia, which
was interpreted as a dependence of the temperature of the ejecta with viewing angle. Our work suggests that (1) a
significant part of these differences in color should be attributed to extinction, (2) this extinction is caused by an
asymmetric distribution of circumstellar material (CSM), and (3) the CSM absorption is generally stronger on the
side of the ejecta opposite to where the ignition occurs. Since it is difficult to explain (3) via any known physical
processes that occur before explosion, we argue that the asymmetry of the CSM is originated after explosion by a
stronger ionizing flux on the side of the ejecta where ignition occurs, probably due to a stronger shock breakout
and/or more exposed radioactive material on one side of the ejecta. This result has important implications for both
progenitor and explosion models.