How Do Type Ia Supernova Nebular Spectra Depend on Explosion Properties? Insights from Systematic Non-LTE Modeling

被引:27
作者
Botyanszki, Janos [1 ]
Kasen, Daniel [1 ,2 ,3 ,4 ]
机构
[1] Univ Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
[2] Univ Calif Berkeley, Dept Astron, 601 Campbell Hall, Berkeley, CA 94720 USA
[3] Univ Calif Berkeley, Theoret Astrophys Ctr, Berkeley, CA 94720 USA
[4] Lawrence Berkeley Natl Lab, Nucl Sci Div, Berkeley, CA 94720 USA
基金
美国国家科学基金会;
关键词
line: formation; radiation mechanisms: nonthermal; radiative transfer; supernovae: general; ELECTRON-ION RECOMBINATION; CLOSE-COUPLING APPROXIMATION; IONIZATION RATE COEFFICIENTS; CHANDRASEKHAR MASS MODELS; DELAYED-DETONATION MODELS; LATE-TIME SPECTRA; WHITE-DWARFS; LIGHT CURVES; SN; 2011FE; ABUNDANCE STRATIFICATION;
D O I
10.3847/1538-4357/aa81d8
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present a radiative transfer code to model the nebular phase spectra of supernovae (SNe) in non-LTE (NLTE). We apply it to a systematic study of SNe Ia using parameterized 1D models and show how nebular spectral features depend on key physical parameters, such as the time since explosion, total ejecta mass, kinetic energy, radial density profile, and the masses of Ni-56, intermediate-mass elements, and stable iron-group elements. We also quantify the impact of uncertainties in atomic data inputs. We find the following. (1) The main features of SN. Ia nebular spectra are relatively insensitive to most physical parameters. Degeneracy among parameters precludes a unique determination of the ejecta properties from spectral fitting. In particular, features can be equally well fit with generic Chandrasekhar mass (Mch), sub-M-Ch, and super-M-Ch models. (2) A sizable (greater than or similar to 0.1 M-circle dot) central region of stable iron-group elements, often claimed as evidence for M-Ch models, is not essential to fit the optical spectra and may produce an unusual flat-top [Co III] profile. (3) The strength of [S III] emission near 9500 angstrom can provide a useful diagnostic of explosion nucleosynthesis. (4) Substantial amounts (greater than or similar to 0.1 M-circle dot) of unburned C/O mixed throughout the ejecta produce [O III] emission not seen in observations. (5) Shifts in the wavelength of line peaks can arise from line-blending effects. (6) The steepness of the ejecta density profile affects the line shapes, offering a constraint on explosion models. (7) Uncertainties in atomic data limit the ability to infer physical parameters.
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页数:17
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