the theoretical understanding of Type Ia Supernovae

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the theoretical understanding of Type Ia Supernovae Daniel Kasen

description

the theoretical understanding of Type Ia Supernovae. Daniel Kasen. SN cosmology. “super-nova”. Supernova Discovery History Asiago Catalog (all supernova types). Proposed. Supernova Factory Lick observatory SN search CfA SN group Carnegie SN project ESSENCE Supernova Legacy Survey. - PowerPoint PPT Presentation

Transcript of the theoretical understanding of Type Ia Supernovae

Page 1: the theoretical understanding of  Type Ia Supernovae

the theoretical understanding of

Type Ia Supernovae

Daniel Kasen

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Supernova Discovery History

Asiago Catalog (all supernova types)

SN cosmology“super-nova”

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Supernova FactoryLick observatory SN searchCfA SN groupCarnegie SN projectESSENCESupernova Legacy Survey

Supernova Discovery Future

Rough predictions and promises…

PanStarrsDark Energy SurveyJDEMLarge Synoptic Survey Telescope (LSST)

ProposedDark Energy Measurements

Systematic error, not statistical error, is the issue (e.g., luminosity evolution)

Aim for Type Ia SNe as reliable standard candles to a few %

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SN Ia ProgenitorsAccreting white dwarf near the Chandrasekhar

limit

Accretion rate:10-7 Msun / year

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White Dwarf IgnitionKuhlen, Woosley, and Glaitzmeier (2006)

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t = 0.0 sect = 0.5 sect = 1.0 sec

3D Deflagration ModelSubsonic turbulent flame burning

t = 1.5 sec

Roepke et al. (2005)

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C/O

boom

Fe

56Ni

Si/S/Ca

C/O

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Type Ia Supernova Light Curves

powered by the beta decay: 56Ni 56Co 56Fe

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Type Ia Supernova Spectrum

20 days after explosion

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Spectroscopic Homogeneity and Diversity

monitoring silicon expansion velocitiesfrom Leonard et al, ApJ 2006

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Type Ia Width-Luminosity Relation

brighter supernovae have broader light curves

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Supernova Ejecta Opacity

blending of millions of line transitions

FeII bound-boundFeIII bound-bound

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free expansion

Light Curves / Spectra(~100 days)

radioactive decay / radiative transfer

Type Iasupernovatheoreticalsimulation challenge

ignition

Presupernova Evolution(~100-109 years)

accreting, convective white dwarf

Explosion (~1-100 secs)

turbulent nuclear combustion / hydrodynamics

Observations

DOE: Scientific Discovery through Advanced Computing (SciDAC)

The “Computational Astrophysics Consortium” (CAC) Stan Woosley (PI)

UC Santa Cruz, UC Berkeley, Stanford, Arizona, Stony Brook, JHU,LANL, LLNL, LBNL

Models

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3-dimensional Time-Dependent Monte Carlo Radiative Transfer

SEDONA CodeExpanding atmosphereRealistic opacitiesThree-dimensionalTime-dependentMulti-wavelengthIncludes spectropolarizationIncludes radioactive decay and gamma-ray transferIterative solution for thermal equilibrium

Kasen et al 2006 ApJ

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Large Scale Computing

Jacquard, NERSC

Incite award, Oak Ridge Lab: 4 million hours/yearAtlas “grand challenge” LLNL: 4 million hours/yearNERSC award, LBL: 3 million hours/year

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Fe

56Ni

Si/S/Ca

C/OGrid of Type Ia Supernova Modelsw/ Stan WoosleySergei BlinikovElena Sorokina

130 one-dimensionalChandrasekhar massmodels with varied composition

ParametersMFe

MNi

MSi

“mixing”MFe + MNi + MSi + Mco = MCH

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Broadband Synthetic Light Curves

Model Compared to observations of SN 2001el

Kasen (2006) ApJ

ParametersMFe = 0.1 Msun MNi = 0.6 Msun

MSi = 0.4 Msun

Kasen, ApJ 2006

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Day 35 after explosion

Time Evolution of Spectrum

Recession of photosphere reveals deeper layers

Fe

56Ni

Si/S/Ca

C/ODay 15 after explosion

ModelSN1994D

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Width-Luminosity Relationship

Kasen and Woosley, ApJ, 2007 Vary 56Ni productionMNi = 0.35 to 0.70 Msun

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The Width-Luminosity Relationship

Kasen and Woosley, ApJ, 2007

Vary 56Ni production

Brighter models are hotter andmore ionized and have different opacity behavior

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The Width-Luminosity Relationship

Kasen and Woosley, ApJ, 2007

Vary 56Ni production

Vary silicon production(explosion energy)

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Multi-Dimensional Models

Roepke et al (2005)

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2D Deflagration Model

MNi = 0.2 Msun

EK = 0.3 x 1051 ergs

Roepke, Kasen, Woosley

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DeflagrationToDetonationKhokhlov (1991)Hoeflich (1994)Gamezo et al (2005)

But how to detonate?

Gamezo et al.

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2D Delayed Detonation

MNi = 0.5 Msun

EK = 1.2 x 1051 ergs

Roepke, Kasen, Woosley

Earlier Detonation (higher densities)gives more 56Ni production

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Off-Center Ignition

University of Chicago FLASH Center

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Detonation From Failed Deflagration Plewa, ApJ (2007)

Is the transition robust in3-dimensional calculations?

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Off-center ExplosionPlewa (2007) Kasen and Plewa (2007)

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Asymmetry and SN Ia Diversity

Maximum Light Spectrum

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Asymmetry and SN Ia Diversity

B-band Light Curve and the Phillips Relation

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How and where does ignition happen?

How might the deflagration transition into a detonation?

Can we reproduce the observed spectra and light curves from first principles?

How do the light curves depend upon progenitor environment?

Pressing Questions

The Theoretical Understanding of Type Ia Supernovae

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