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Published byKathryn Lindsey Modified over 9 years ago
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SNLS-03D3bb Andy Howell University of Toronto and the Supernova Legacy Survey (SNLS)
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Host z = 0.2440 HST CFHT From PEGASE 2 fits to host ugriz photometry: M yr -1 Formally implies host age of 0.7 Gyr, though highly uncertain
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Si II velocity Low-z data from Benetti et al. 2005
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Lightcurve V=20.5 ± 0.06 M V = -19.94 ± 0.06 Use only r, i fit s = 1.13 Sparse LC from early days of survey
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V magnitude distribution M V = -19.94 ± 0.06 Low-z Astier et al. sample 2.2 times the luminosity of median SN Ia
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56 Ni mass erg s -1 M -1 Arnett’s rule: Luminosity at maximum is proportional to spontaneous energy deposition by radioactive decay. : ratio of bolometric to radioactivity luminosities : energy per second per solar mass from radioactive deacay Using t r = -19.5 (Conley et al. 2006), = 1.2 (Nugent et al. 1996), get M Ni = 1.29 ± 0.07 M
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Velocity from kinetic energy Energy from burning to Fe peak: erg s -1 M -1 3 kinds of elements: Fe-peak, IME, unburned C/O KE is nuclear energy minus binding energy Burning to Si produces 76% as much 56 Ni is 70% of Fe-peak elements: Binding energy (Yoon & Langer 2005) - 1.4 M WD: 0.5e51 erg - 2.0 M WD: 1.3e51 erg
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Implications - Progenitors Double degenerate model: merger of two massive WDs can produce super- Chandra product. In youngest populations, only massive WDs exist. Before 0.9 Gyr, combined WD mass must be > Chandrasekhar mass. Single degenerate model: rapid rotation could support 2 solar mass WD according to Yoon & Langer 2005. Young pop. favored for higher starting WD, secondary masses.
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Implications The most luminous SNe occur in young populations Super-Chandra model predicts more luminous SNe in younger populations Chandra model has no explanation for this. Could WD mass partially drive luminosity fluctuations in SNe Ia?
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Conclusions - Observations M V =19.94 ± 0.06, brightest SN Ia ever observed (with the possible exception of the interacting SN 2002ic) SiII velocity at +2d among the lowest seen, 8000 km/s SiII strong relative to CaII at +2d, in contrast with other SNe Ia CII near maximum implies the presence of unburned material deep into the SN Low-mass, blue host implies a young progenitor age
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Conclusions - Interpretation Arnett’s law implies ~1.3 M 56 Ni. If ~40% of elements are non- 56 Ni, M WD ~ 2.1 M High 56 Ni mass implies large nuclear energy, which should produce large velocities in Chandrasekhar model. Low velocity consistent with increased binding energy of super-Chandra model. Young galaxy consistent with expectations from Super-Chandra model SNLS-03D3bb meets every expectation of the super- Chandra model
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Conclusions - Cosmology WD mass may partially drive SN Ia luminosity SNLS-03D3bb does not follow stretch- luminosity relationship (it is too bright by 4.4 sigma). “Evolution” in SNe with redshift? SNLS-03D3bb was thrown out of Astier et al. (2006), but less extreme examples could be in data set.
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Time to evolve off main sequence
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What mass WD does a star make? Ferrario et al. 2005
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UV – metallicity effects?
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Velocity vs. WD mass
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B-V color
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V-R color
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