From Z=0 to Z=0.02 Type Ia SN Progenitors: Any influence on LCs ?? SNIa: Where we are ?? Inma Domínguez Group of Stellar Evolution and Nucleosynthesis Universidad de Granada Peter Höflich, University of Texas, USA Oscar Straniero, L. Piersanti, A. Tornambe, Osservatorio di Teramo, Italy F. Brachwitz, F.K. Thielemann, Univ. of Basel, Switzerland E. Bravo, UPC, Barcelona Cosmic Concordance Ωm~ 0.3 Ωλ ~ 0.7 Ho = 65 km/s/Mpc Age of the Universe 14000 Myr SNe at z~0.4-0.8: 0.25 mag fainter than for an EMPTY Universe Fainter x Further High-z Team SN Cosmology Project SN Ia are NOT equal ∆MMAX ~ 3 mag Results are based on Empirical Relations MMAX Q LC shape Calibrated Locally !!! Systematic effects MAX-LC Shape Relations MLCS: Correlation MMAX Q Peak width LC: 56Ni x 56Co x56 Fe MMAX ∝ MNi (Arnett 1982) Brighter Slower Decline Dimmer Faster Decline Riess et al. , 1997 Maximum Brightness - Decline Relation Phillips et al. 1996, 1999 Mmax-∆m15 <σ> = 0.17 mag ∆m15 Caution: local calibrations Correlation with host galaxy morphology Hamuy et al., 2000 Ivanov et al. 2000 Brighter SNIa in Spirals Galaxies Hamuy et al. , 1995, 1996 Branch et al. 1996 Caution !! SNe related with Ì Populations ?? but Mmax Q ∆m15 independent of galaxy morphology Few objects More observations !! SNe Statistics SN rate per unit Mass [10-11 M 10-2 yr x (Ho/65)2] Galaxy SN Ia E-S0 0.12±0.02 S0a-Sb 0.22±0.05 S0c-Sd 0.35±0.08 Cappellaro, Barbon, Turatto 2003 SN Ia Rate 3 times y in late Spiral Galaxies Caution !! Part of SN Ia comes from a younger population ? Evolutionary effects ?? Stellar Population Progenitor Light Curve Still … Key Problems !! ¾ Progenitors ? MCh CO WD companion ?? ¾ Explosion Mechanism ? begin subsonic 1D parametrization of the Deflagration velocity 3D still NOT a sucessfull explosion ¾ How stellar populations evolve with z ??!! Numerical Methods 9 STELLAR EVOLUTION: FRANEC (Chieffi, Cristallo, Domínguez, Imbriani, Limongi, Straniero) 1D Hydrostatic Code ¾ Extended Nuclear Network (500 isotopes) ¾ Physics and Chemestry coupled ¾ Time dependent mixing 9 EXPLOSION & LIGHT CURVES 1D Radiation-Hydrodynamic Code (PPM) ¾ Extended Nuclear Network (Höflich, Khokhlov) ¾ γ Ray transport Monte Carlo ¾ 3D simulations velocity of deflagration (Domínguez, Höflich) Mch Delayed Detonations Explosions LC, spectra, Mmax Q ∆M15 56Ni ρtr Mmax Q ∆M15 ρtr : 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.3 2.5 2.7 x 107 g/cm3 ρtr shorter pre-expansion ρburn 56Ni IME (Ca, S, Si, Mg) Ek ≈ Dependence on the initial Z LCs M=5 M (1.5 7 M) Z 10-10 C/O WD 10-3 (fuel) 0.02 C/OCh MNi (M) Up to ∆MMAX =0.05 mag 0.70 0.55 No dependence of MMAX with initial Z 0.66 0.54 Domínguez et al. 2001 0.72 0.56 Spectra at Max. (high velocities) Fe lines opacity Z κ Flux U UV B B-V (bluer) ∆(B-V) < 0.07 Extinction ∆MMAX < 0.2 mag Höflich, Wheeler,Thielemann, 1998 Other results on Z... ¾ Umeda et al. (1999) & Iwamoto el al. (1999) DO find a dependence of C/O with Z ¾ Timmes et al. (2003) confirm our results for Z< 0.02 but finds a “strong” dependence for Z>0.02 (Ni mass) 0.6 Timmes et al. MNi (M) 0.2 0.1 Z(Z ) 0.02 10 Röpke & Hillebrandt (2004) in 3D simulations find that the 56Ni mass does not depend on C/O • Strong mix • Not all the WD is burnt Dependence on initial MMS (age) C/O WD LCs MMS 1.5 5.0 7.0 Z=0.02 C/OCh MNi (M) 0.75 0.59 0.72 0.56 0.60 0.52 Up to ∆MMAX = 0.2 mag Correlated with vph & trise Domínguez et al. 2001 Explosive conditions from Ì evolution Rotation Piersanti et al. 2003 Expected ∆MMAX < 0.2 mag Domínguez et al. 2004 Conclusions ¾ The Majority of SNIa D STANDARD BOMBS ¾ ∆MMAX ~ 3 mag D related with population ? (obs.) due to MNi (models) It is already included in the Mmax-∆m15 !!! ¾ Peculiar events may be identified by the spectrum D take good ones at high z !! ¾ Our Study about the influence of Progenitors: MMS (age) ρc (WD cooling, accretion) Rotation Z D Extinction correction ∆MMAX < 0.2 mag ∆MMAX = 0.2 mag is relevant for Ωλ ?? within errors Knop et al. (2003) ΩT=1 w=cte P = wρ ρ ∝ R −3( w+1) Vacuum energy Not for the Existence !! Sí for its Nature (?) ∆MMAX < 0.05 - 0.1 mag
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