supernovae of type ia

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LSU - 25 Oct 07 1 Supernovae of Type Ia Supernovae of Type Ia Ronald F. Webbink Department of Astronomy University of Illinois SN 1994D in NGC 4526 (HST)

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Supernovae of Type Ia. Supernovae of Type Ia. Ronald F. Webbink Department of Astronomy University of Illinois. SN 1994D in NGC 4526 (HST). Supernova taxonomy. www.astronomy.com. Hachinger et al. 2006. Cosmological significance. SNe Ia as standard candles - PowerPoint PPT Presentation

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Page 1: Supernovae of Type Ia

LSU - 25 Oct 07 1

Supernovae of Type Ia

Supernovae of Type Ia

Ronald F. Webbink

Department of Astronomy

University of Illinois

SN 1994D in NGC 4526 (HST)

Page 2: Supernovae of Type Ia

LSU - 25 Oct 07 2Hachinger et al. 2006

Supernova taxonomy

www.astronomy.com

Page 3: Supernovae of Type Ia

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Cosmological significance

• SNe Ia as standard candles

• Magnitude => Expansion of light sphere with respect to comoving coordinates

• Redshift => Expansion of comoving coordinates

Wood-Vasey, et al. 2007

Page 4: Supernovae of Type Ia

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All SNe Ia are

not the same

www.nd.edu/~kkrisciu

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• What is the physical cause of this dispersion?

• Is it truly independent of redshift?

• What secondary factors should affect SN Ia properties?

=> Physics of supernova explosions

• What are their progenitors?

www.nd.edu/~kkrisciu

Page 6: Supernovae of Type Ia

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What do we know?

• Occur in both spiral and elliptical galaxies

Li 2007

Page 7: Supernovae of Type Ia

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What do we know?

• Occur in both spiral and elliptical galaxies

• Rate in spirals correlates with star formation rate (prompt component)

McMillan & Ciardullo 1996

Page 8: Supernovae of Type Ia

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What do we know?

• Occur in both spiral and elliptical galaxies

• Rate in spirals correlates with star formation rate (prompt component)

• Persistent rate among passive (elliptical) galaxies (delayed component)

Sullivan et al. 2006

Page 9: Supernovae of Type Ia

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What do we know?

• Speed correlates with galaxy type

Gallagher et al. 2005

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What do we know?

• Speed correlates with galaxy type

• No H, He => MCSM < ~0.03 Msun

Lundqvist 2007

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What do we know?

• Speed correlates with galaxy type

• No H, He => MCSM < ~0.03 Msun

• Radio- and X-ray non-detections => dM/dt < ~10-7 Msun yr-1

Panagia, et al. 2006

Hughes et al. 2007

Page 12: Supernovae of Type Ia

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What do we know about the progenitors?• White dwarf progenitors

No H, He

Some SNe Ia from old stellar populations

Page 13: Supernovae of Type Ia

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What do we know about the progenitors?• White dwarf progenitors

No H, He

Some SNe Ia from old stellar

populations

• Thermonuclear runawaySpectra

No compact remnants found

Stehle, et al. 2005

Page 14: Supernovae of Type Ia

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What do we know about the progenitors?• White dwarf progenitors

No H, He

Some SNe Ia from old stellar

populations

• Thermonuclear runawaySpectra

No compact remnants found

• Powered by 56Ni to 56Co

to 56Fe decaySpectra

Light curves Röpke et al. 2007

Page 15: Supernovae of Type Ia

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What do we know about the progenitors?• White dwarf progenitors

No H, He

Some SNe Ia from old stellar populations

• Thermonuclear runawaySpectra

No compact remnants found

• Powered by 56Ni to 56Co to 56Fe decaySpectra

Light curves

• Binary systemsNo other plausible way to trigger instability

Page 16: Supernovae of Type Ia

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Common envelope evolution

Yungelson 2007

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Stable mass transfer

Yungelson 2007

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SN Ia Progenitors

Yungelson 2007

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Candidate Progenitors• Single Degenerates

Cataclysmic VariablesRecurrent NovaeSymbiotic StarsSupersoft X-ray Sources

• Edge-Lit DetonationssdHe/HeWD + CO WD

• Double DegeneratesCO + CO White Dwarfs

Page 20: Supernovae of Type Ia

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Cataclysmic Variables

• Outbursting binaries: Classical Novae (CN)

Dwarf novae (DN)

Novalike variables (NL)

Magnetic CVs (MCV)

• Mwd ~ 0.6-1.0 Msun

• Mdonor < ~2/3 – 1 Msun

• Accretion events (DN,

NL, MCV)

• dM/dt ~ 10-11 – 10-8 Msun yr-1

• Pcrit ~ 1019 dyne cm-2

=> Thermonuclear runaway

Page 21: Supernovae of Type Ia

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Nova ignition masses

Townsley & Bildsten 2005

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Gehrz et al. 1998

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Classical nova outbursts

• Runaways erode Mwd!

• Many classical novae contain ONeMg white dwarfs

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Recurrent Novae

• Mwd close to MCh

• Ejecta lack the heavy-element enhancements characteristic of classical novae => dMwd/dt > 0 ?

• Core composition unknown, but likely to be ONeMg white dwarfs (cf. CN)

• Rare: Death rate ~ 10-2 SN Ia rate

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Symbiotic Stars

• Heterogenous class of objects, mostly wind-accreting WD companions to luminous M giants or AGB stars

• Hot components mostly powered by H burning on white dwarf

• Mwd mostly unknown, but those in T CrB, RS Oph (erstwhile RNe) must be near MCh

• Extremely H-rich environment

Page 26: Supernovae of Type Ia

LSU - 25 Oct 07 26Munari & Zwitter 2002

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Supersoft X-ray Sources

• Heterogeneous class of objects (incl. PNNe, SNR, Symbiotic Stars), but many are stable H-burning white dwarfs

Nomoto et al. 2007

Page 28: Supernovae of Type Ia

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Supersoft X-ray Sources

• Heterogeneous class of objects (incl. PNNe, SNR, Symbiotic Stars), but many are stable H-burning white dwarfs

• Population synthesis predicts ~103 SSS in M31 if SN Ia progenitors

Page 29: Supernovae of Type Ia

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SSS in M31

center disk

Di Stefano 2007

Page 30: Supernovae of Type Ia

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Supersoft X-ray Sources

• Heterogeneous class of objects (incl. PNNe, SNR, Symbiotic Stars), but many are stable H-burning white dwarfs

• Population synthesis predicts ~103 SSS in M31 if SN Ia progenitors => 102 times number seen in X-rays

• Can they be hidden?

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Evolution of SSS

Di Stefano & Nelson 1996

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Supersoft X-ray Sources• Can they be hidden?

• Perhaps super-Eddington luminosity (accretion + burning) drives a massive stellar wind

Hachisu & Kato 2003

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Supersoft X-ray Sources• Can they be hidden?

• Perhaps super-Eddington luminosity (accretion + burning) drives a massive stellar wind

• BUT such a model predicts– H, He-rich ejecta

– Relatively dense stellar wind

both in violation of observational limits

Page 34: Supernovae of Type Ia

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Supersoft X-ray Sources• Can they be hidden?

• Perhaps super-Eddington luminosity (accretion + burning) drives a massive stellar wind

• BUT such a model predicts– H, He-rich ejecta

– Relatively dense stellar wind

both in violation of observational limits

• Alternative: Super-Eddington accretion regenerates AGB giant

Page 35: Supernovae of Type Ia

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Supersoft X-ray Sources• Can they be hidden?

• Perhaps super-Eddington luminosity (accretion + burning) drives a massive stellar wind

• BUT such a model predicts– H, He-rich ejecta

– Relatively dense stellar wind

both in violation of observational limits

• Alternative: Super-Eddington accretion regenerates AGB giant

• Maximum lifetime to carbon ignition (delay to SN Ia) ~ 1.6 X 109 yr

Page 36: Supernovae of Type Ia

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Problems withSingle-Degenerate Progenitors

• Instability of He-burning shell

Page 37: Supernovae of Type Ia

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Thermal pulses in AGB stars

Iben & Renzini 1983

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Thermal pulses in accreting white dwarfs

Cassisi, Iben & Tornambè 1998

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Problems withSingle-Degenerate Progenitors

• Instability of He-burning shell– What of Surface Hydrogen Burning?

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Surface Hydrogen Burning

Starrfield 2007

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Surface Hydrogen Burning

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Problems withSingle-Degenerate Progenitors

• Instability of He-burning shell• Ablation of H-rich donor in supernova event

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Marietta, Burrows & Fryxell 2000

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Problems withSingle-Degenerate Progenitors

• Instability of He-burning shell• Ablation of H-rich donor in supernova event• Surviving companion?

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Companion peculiar velocities

Canal, Méndez & Ruiz-Lapuente 2001

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Tycho (SN1572) Companion?

Ruiz-Lapuente, et al. 2004

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Companion Rotation Velocities

Schmidt 2007

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Tycho G revisited

Schmidt 2007

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Edge-Lit Detonations• Degenerate ignition of ~0.1 Msun of He on ~1 Msun

CO white dwarf can trigger double detonation• Mass transfer too rapid from non-degenerate He

star donor to permit accreted envelope to cool to degeneracy and develop strong flashes

• Degenerate donors have even higher mass transfer rates until Mdonor < ~0.05 Msun

• Degenerate He ignition produces outward-propagating detonation, but fails to detonate CO core, or to produce intermediate-mass elements (e.g., Si) seen at maximum light

Page 51: Supernovae of Type Ia

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Failed Double Detonation

Bildsten 2007

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CO +CO White Dwarf Mergers

• Wide range of delay times from GR inspiral

Yungelson 2007

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CO +CO White Dwarf Mergers

• Wide range of delay times from GR inspiral

• Eddington-limited accretion ignites carbon at the base of the accreted envelope (1D)

Nomoto & Iben 1985

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CO +CO White Dwarf Mergers

• Wide range of delay times from GR inspiral

• Eddington-limited accretion ignites carbon at the base of the accreted envelope (1D)

• But mass transfer occurs on a dynamical time scale

Page 55: Supernovae of Type Ia

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White dwarf coalescence

Yoon, Podsiadlowski & Rosswog 2007

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Merged Double White Dwarf

Yoon, Podsiadlowski & Rosswog 2007

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CO +CO White Dwarf Mergers

• Wide range of delay times from GR inspiral

• Eddington-limited accretion ignites carbon at the base of the accreted envelope (1D)

• But mass transfer occurs on a dynamical time scale

• Carbon ignition quenched in 2D or 3D by meridional expansion

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Problems withDouble-Degenerate Progenitors

• Tidal synchronization and preheating during approach to merger

Iben, Tutukov & Fedorova 1998

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Problems withDouble-Degenerate Progenitors

• Tidal synchronization and preheating during approach to merger

• Angular momentum transport

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Synchronization at low accretion rates

• KH – Kelvin-Helmholtz instability

• BC – Baroclinic instability

• TS – Tayler-Spruit dynamo

Piro 2007

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Problems withDouble-Degenerate Progenitors

• Tidal synchronization and preheating during approach to merger

• Angular momentum transport

• Shock heating of accreted matter and the site of carbon ignition

=> Neutrino cooling of accreted envelope?

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Are there enough double-degenerates?

Napiwotzki 2007

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Theoretical DD Search Yields

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SN Ia ProgenitorComparative Yields

Yungelson 2007

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The Parting Shot:We’re looking for haystacks, not needles!

Maoz 2007