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LIBRIS Formathandbok  (Information om MARC21)
FältnamnIndikatorerMetadata
00004168naa a2200649 4500
001oai:DiVA.org:su-159008
003SwePub
008180910s2018 | |||||||||||000 ||eng|
024a https://urn.kb.se/resolve?urn=urn:nbn:se:su:diva-1590082 URI
024a https://doi.org/10.3847/1538-4357/aacb352 DOI
040 a (SwePub)su
041 a engb eng
042 9 SwePub
072 7a ref2 swepub-contenttype
072 7a art2 swepub-publicationtype
100a Bose, Subhash4 aut
2451 0a ASASSN-15nx :b A Luminous Type II Supernova with a Perfect Linear Decline
264 c 2018-07-27
264 1b American Astronomical Society,c 2018
338 a print2 rdacarrier
520 a We report a luminous Type II supernova, ASASSN-15nx, with a peak luminosity of M-v = -20 mag that is between those of typical core-collapse supernovae and super-luminous supernovae. The post-peak optical light curves show a long, linear decline with a steep slope of 2.5 mag (100 day)(-1) (i.e., an exponential decline in flux) through the end of observations at phase approximate to 260 day. In contrast, the light curves of hydrogen-rich supernovae (SNe II-P/L) always show breaks in their light curves at phase similar to 100 day, before settling onto Co-56 radioactive decay tails with a decline rate of about 1 mag (100 day)(-1). The spectra of ASASSN-15nx do not exhibit the narrow emission-line features characteristic of Type IIn SNe, which can have a wide variety of light-curve shapes usually attributed to strong interactions with a dense circumstellar medium (CSM). ASASSN-15nx has a number of spectroscopic peculiarities, including a relatively weak and triangular-shaped H alpha emission profile with no absorption component. The physical origin of these peculiarities is unclear, but the long and linear post-peak light curve without a break suggests a single dominant powering mechanism. Decay of a large amount of Ni-56 (M-Ni = 1.6 +/- 0.2 M-circle dot) can power the light curve of ASASSN-15nx, and the steep light-curve slope requires substantial gamma-ray escape from the ejecta, which is possible given a low-mass hydrogen envelope for the progenitor. Another possibility is strong CSM interactions powering the light curve, but the CSM needs to be sculpted to produce the unique light-curve shape and avoid producing SN IIn-like narrow emission lines.
650 7a NATURVETENSKAPx Fysikx Astronomi, astrofysik och kosmologi0 (SwePub)103052 hsv//swe
650 7a NATURAL SCIENCESx Physical Sciencesx Astronomy, Astrophysics and Cosmology0 (SwePub)103052 hsv//eng
653 a supernovae: general
653 a supernovae: individual (ASASSN-15nx)
700a Dong, Subo4 aut
700a Kochanek, C. S.4 aut
700a Pastorello, Andrea4 aut
700a Katz, Boaz4 aut
700a Bersier, David4 aut
700a Andrews, Jennifer E.4 aut
700a Prieto, J. L.4 aut
700a Stanek, K. Z.4 aut
700a Shappee, B. J.4 aut
700a Smith, Nathan4 aut
700a Kollmeier, Juna4 aut
700a Benetti, Stefano4 aut
700a Cappellaro, E.4 aut
700a Chen, Ping4 aut
700a Elias-Rosa, N.4 aut
700a Milne, Peter4 aut
700a Morales-Garoffolo, Antonia4 aut
700a Tartaglia, Leonardou Stockholms universitet,Institutionen för astronomi,Oskar Klein-centrum för kosmopartikelfysik (OKC)4 aut0 (Swepub:su)leta1160
700a Tomasella, L.4 aut
700a Bilinski, Christopher4 aut
700a Brimacombe, Joseph4 aut
700a Frank, Stephan4 aut
700a Holoien, T. W. -S.4 aut
700a Kilpatrick, Charles D.4 aut
700a Kiyota, Seiichiro4 aut
700a Madore, Barry F.4 aut
700a Rich, Jeffrey A.4 aut
710a Stockholms universitetb Institutionen för astronomi4 org
773t Astrophysical Journald : American Astronomical Societyg 862:2q 862:2x 0004-637Xx 1538-4357
856u https://arxiv.org/pdf/1804.00025.pdf
8564 8u https://urn.kb.se/resolve?urn=urn:nbn:se:su:diva-159008
8564 8u https://doi.org/10.3847/1538-4357/aacb35

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