1995
DOI: 10.1086/175656
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Delayed detonation models for normal and subluminous type IA sueprnovae: Absolute brightness, light curves, and molecule formation

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Cited by 251 publications
(308 citation statements)
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“…Similar trends appear in the J, H, and K-band LC (Krisciunas et al 2004b), although interesting exceptions have been sought out (e.g., SN 2000cx Candia et al 2003). Despite the theoretical insights (e.g., Hoflich et al 1995;Wheeler et al 1998;Pinto & Eastman 2000a,b;Kasen 2006), the origin of the NIR secondary maximum and its dependence on the SN ejecta properties remain unclear. These NIR LCs therefore provide promising means of investigating a possible empirical secondary parameter, which may explain the deviations from the standard width-luminosity relation (Kasen 2006), and thus help us to understand the intrinsic differences among SNe Ia.…”
Section: Introductionmentioning
confidence: 80%
“…Similar trends appear in the J, H, and K-band LC (Krisciunas et al 2004b), although interesting exceptions have been sought out (e.g., SN 2000cx Candia et al 2003). Despite the theoretical insights (e.g., Hoflich et al 1995;Wheeler et al 1998;Pinto & Eastman 2000a,b;Kasen 2006), the origin of the NIR secondary maximum and its dependence on the SN ejecta properties remain unclear. These NIR LCs therefore provide promising means of investigating a possible empirical secondary parameter, which may explain the deviations from the standard width-luminosity relation (Kasen 2006), and thus help us to understand the intrinsic differences among SNe Ia.…”
Section: Introductionmentioning
confidence: 80%
“…At the time of the explosion of the WD, its central density ρ c is 2.0 × 10 9 g cm −3 and its mass is close to 1.37 M . The transition density ρ tr has been identified as the main factor that determines the 56 Ni production, and thus the brightness of a SNe Ia (Höflich 1995;Höflich et al 1995;Iwamoto et al 1999). The deflagration-to-detonation transition density is ρ tr = 8 × 10 6 g cm −3 .…”
Section: Delayed-detonation Modelmentioning
confidence: 99%
“…The ratio depends strongly on wavelength. P as a function of the inclination for a source located off-center, at a distance D = R ph /R of 3 (solid blue) and 1.5 (dotted red) (adopted from Höflich et al 1995). Note that D = 3 corresponds to SN 2005ke at day −8, when the photosphere R ph is formed at about 10 000 km s −1 , and assuming the maximum off-center 56 Ni distribution suggested by Maeda et al (2011) for core-normal SNe Ia.…”
Section: Continuum Polarizationmentioning
confidence: 99%
“…The secondary maximum was first noted by Elias et al (1981). Höflich et al (1995) explained the secondary maximum as due to the expansion of the IR pseudophotosphere, whereas Suntzeff (1996) suggested that it was due to a global shift of radiation from blue to red. Pinto & Eastman (2000) suggested that the transition from Fe III to Fe II as the dominant ionization stage was important although they implied that the secondary maximum occurs when the photosphere has receded into the non-radioactive center.…”
Section: Introductionmentioning
confidence: 99%