Exploring the diffusion induced nova scenario

Slides:



Advertisements
Similar presentations
Stellar Structure Section 6: Introduction to Stellar Evolution Lecture 18 – Mass-radius relation for black dwarfs Chandrasekhar limiting mass Comparison.
Advertisements

PHYS The Main Sequence of the HR Diagram During hydrogen burning the star is in the Main Sequence. The more massive the star, the brighter and hotter.
Sakurai’s Object Dr H F Chau Department of Physics HKU Dr H F Chau Department of Physics HKU A Case Of Superfast Stellar Evolution.
The Standard Solar Model and Its Evolution Marc Pinsonneault Ohio State University Collaborators: Larry Capuder Scott Gaudi.
Asymptotic Giant Branch. Learning outcomes Evolution and internal structure of low mass stars from the core He burning phase to the tip of the AGB Nucleosynthesis.
The importance of the remnant’s mass for VLTP born again times Marcelo Miguel Miller Bertolami Part of the PhD thesis work (in progress) under the supervision.
Chapter 12 Stellar Evolution. Infrared Image of Helix Nebula.
Chemical evolution of Super-AGB stars The Giant Branches Lorentz Center, May 2009 Enrique García-Berro 1,2 1 Universitat Politècnica de Catalunya 2 Institut.
Post Main Sequence Evolution PHYS390 (Astrophysics) Professor Lee Carkner Lecture 15.
Post-AGB evolution. Learning outcome evolution from the tip of the AGB to the WD stage object types along the post-AGB evolution basics about planetary.
Lecture 15PHYS1005 – 2003/4 Lecture 16: Stellar Structure and Evolution – I Objectives: Understand energy transport in stars Examine their internal structure.
ATON code for stellar evolution for stellar evolution Italo Mazzitelli (IAS - Rome) Francesca D’Antona (Observatory of Rome) Paolo Ventura (Observatory.
Stellar Winds and Mass Loss Brian Baptista. Summary Observations of mass loss Mass loss parameters for different types of stars Winds colliding with the.
Ch. 11: The Deaths and Remnants of Stars (part a) The evolution of intermediate-mass stars. Planetary nebulae and the formation of white dwarf stars. Supernova.
Lecture 1 Time Scales, Temperature-density Scalings, Critical Masses.
The Death of a Low Mass Star n Evolution of a sun-like star post helium- flash –The star moves onto the horizontal branch of the Hertzprung-Russell diagram.
The white dwarf cooling age of NGC 6791 Enrique García-Berro, Santiago Torres, Leandro Althaus, Isabel Renedo, Pablo Lorén-Aguilar, Alejandro.
The Sun... And Other Stars! Star Classification:.
Stellar Evolution. Consider a cloud of cold (50 deg K) atomic hydrogen gas. If an electron of one atom flips its spin state and the electron then has.
Announcements Exam 3 is scheduled for Wednesday April 8. Will be pushed back to Monday April 13 Tentatively will cover the rest of Chapter 4 and all of.
Lecture 17 Post-ms evolution II. Review Review Review.
Composition and Mass Loss. 2 Two of the major items which can affect stellar evolution are Composition: The most important variable is Y – the helium.
Garching, 19/05/20041 Modelling the PNLF: Population Effects on the Bright Cut-off Paola Marigo – Dipartimento di Astronomia,Padova Léo Girardi – Osservatorio.
A Star Becomes a Star 1)Stellar lifetime 2)Red Giant 3)White Dwarf 4)Supernova 5)More massive stars October 28, 2002.
Yields from single AGB stars Amanda Karakas Research School of Astronomy & Astrophysics Mt Stromlo Observatory.
Quiz #6 Most stars form in the spiral arms of galaxies Stars form in clusters, with all types of stars forming. O,B,A,F,G,K,M Spiral arms barely move,
A note on: Group Behavior Open Clusters: contain a few hundred to a few thousands of stars. Lie in the plane of the Milky Way Galaxy. A few parsecs in.
9. Evolution of Massive Stars: Supernovae. Evolution up to supernovae: the nuclear burning sequence; the iron catastrophe. Supernovae: photodisintigration;
African Savanna
Classical Novae on a Helium White Dwarf Irit Idan (Technion) Lars Bildsten ((KITP, UCSB) Ken Shen (UCSB)
Tübingen, Hydrogen-Deficient Stars1 O(He) Stars Thomas Rauch Elke Reiff Klaus Werner Jeffrey W. Kruk Institute for Astronomy and Astrophysics.
Death of sun-like Massive star death Elemental my dear Watson Novas Neutron Stars Black holes $ 200 $ 200$200 $ 200 $ 200 $400 $ 400$400 $ 400$400.
18-19 Settembre 2006 Dottorato in Astronomia Università di Bologna.
The Chemistry of PPN T. J. Millar, School of Physics and Astronomy, University of Manchester.
Tubingen, September, Optical spectroscopy of the born- again Sakurai's object in 1996 Igor Savanov Simon Jeffery Don Pollacco Denis Shulyak.
Chapter 12: Stellar Evolution. Most stars spend a majority of their lives (~90%) on the main sequence (about 10 billion years for our Sun) Virtually all.
High energy Astrophysics Mat Page Mullard Space Science Lab, UCL 7. Supernova Remnants.
On The Fate of a WD Highly Accreting Solar Composition Material Irit Idan 1, Nir J. Shaviv 2 and Giora Shaviv 1 1 Dept. Of Physics Technion Haifa Israel.
The Future of White Dwarf Asteroseismology Travis Metcalfe (NCAR) NGC 1514 – Crystal Ball Nebula.
Exploring the diffusion induced nova scenario Marcelo Miguel Miller Bertolami Leandro Gabriel Althaus (FCAGLP-UNLP/IALP CONICET, Argentina) Exploring the.
CSI661/ASTR530 Spring, 2011 Chap. 2 An Overview of Stellar Evolution Feb. 23, 2011 Jie Zhang Copyright ©
Convective Core Overshoot Lars Bildsten (Lecturer) & Jared Brooks (TA) Convective overshoot is a phenomenon of convection carrying material beyond an unstable.
Objectives: To learn what defines a Main sequence star
The Adventures of a Thermally Pulsating AGB Star
Stars on and off the Main Sequence
Star Formation - 6 (Chapter 5 – Universe).
Mariko KATO (Keio Univ., Japan) collaboration with
Stellar Evolution Chapters 16, 17 & 18.
Exoplanet Host Stars.
HST/COS Observations of O(He) Stars
25.2 – Stellar Evolution – Part II
Contents of the Universe
How Stars Evolve Pressure and temperature The fate of the Sun
Annoucements Next test is in one week
Stellar Evolution Chapter 19.
Evolution off the Main Sequence
Life Cycle of a Star Star Life Cycle: Stars are like humans. They are born, live and then die.
Chapter 21 Galaxy Evolution
How Stars Evolve Pressure and temperature The fate of the Sun
Goals Explain why stars evolve Explain how stars of different masses evolve Describe two types of supernova Explain where the heavier elements come from.
Homework #6: due Friday, March 23, 5pm
Lecture 23: Stellar Life-Cycles.
The Deaths of Stars.
The Giant Branches Workshop - Lorentz Center,
ASTEROSEISMOLOGY OF LATE STAGES OF STELLAR EVOLUTION
Low Mass Stars (< 8 MSun) - Outline
Stellar Evolution.
The structure and evolution of stars
Astronomy Chapter VII Stars.
Composition and Mass Loss
Presentation transcript:

Exploring the diffusion induced nova scenario Marcelo Miguel Miller Bertolami Leandro Gabriel Althaus (FCAGLP-UNLP/IALP CONICET, Argentina) Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Publicity: La Plata White Dwarf Models (LPCODE) Updated physics, realistic pre-white dwarf evolution, time dependent diffusion, colors and much more! Tracks available at http://www.fcaglp.unlp.edu.ar/evolgroup/tracks.html in two different flavors: H-rich: Renedo et al. 2010, ApJ, 717, 183 H-deficient: Althaus et al. 2009, ApJ, 704, 1605 See poster by Renedo et al. ! Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Diffusion Induced Novas (a.k.a. Self Induced Novas) ●Iben & MacDonald (1986) Diffusion triggered CNO flash at Teff~40000 K Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Objectives Motivation ●Although mentioned in several reviews and articles (D’Antona & Mazzitelli 1990, Iben 1995, Hansen 2003, Lawlor & MacDonald 2006 Kalirai et al 2007, Althaus et al. 2010), first and only simulation of the event dates from 25 years ago. (later: white dwarf models were criticized for not being realistic enough) ●Iben & MacDonald made several predictions/speculations: The star becomes a yellow giant a few years after the CNO-flash Its surface abundance is mildly He-enriched with NH/NHe ~1 Diffusion induced novas occur when ΔMbuffer < ΔMH /10 The star luminosity brightens 10 mag, light curve look like very slow nova Diffusion induced novas are expected to be recurrent H-burning and strong winds during the giant phases will lead to H-depletion of the star, leading to the formation of non-DA white dwarfs ●Diffusion induced novas might lead to very thin H-envelopes as those predicted by some asteroseismological studies of DAV (see Castanheira & Kepler 2009). Objectives Find if diffusion induced novas occur in realistic white dwarf models. If so, find under which conditions diffusion induced novas occur (thin He-buffers). Find if diffusion induced novas can lead to DAs with thin H-envelopes Make predictions on its surface abundances and expansion times (light curves) Compare with Iben & MacDonald predictions/speculations Think/speculate about possible observational counterparts Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Evolutionary Scenario: Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Modeling (some key points): Pre-white dwarfs evolution In order to produce realistic white dwarf models we computed “cradle to grave” evolutionary sequences following the evolution from the ZAMS through the TP-AGB phase Standard AGB mass loss prescriptions were adopted during the AGB evolution and during the final He-shell flash (exception: some tuning of mass loss to obtain desired type of final flash) No extramixing (overshooting) included at the base of the convective envelope and the He-shell flash convective zone. No (strong) third dredge up is present in low mass AGB stars in agreement with the Initial Final Mass Function (Salaris et al. 2009) and observations of carbon stars (Guandalini et al. 2007) We followed 16 nuclear species with a detailed nuclear network. Nuclear burning and convective mixing are solved simultaneously. Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Modeling (some key points): The White Dwarf phase Time-dependent diffusion was considered. In particular we consider gravitational settling, thermal and chemical diffusion (no radiative levitation). This is done within the multicomponent gas treatment of Burgers (1969) and solved like in Iben & MacDonald (1985): Equations of state: Segretain (1994, high density regime), Magni & Mazzitelli (1979, updated 1993, low density regime) Conductive opacities: Cassisi et al. (2007) Radiative opacities: Iglesias & Rogers (1996) + Alexander & Ferguson (1994) consistent with the metal content of each layer predicted by time-dependent diffusion Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Results: A diffusion induced nova Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Results: A diffusion induced nova : Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Results: Predicted Properties: Timescales, abundances, etc. Main Facts: -White dwarf age at the moment of CNO-flash (1): 106 - 108 years -Expansion times (2): 2 - 10 years -Reheating time: from ~50 to ~400 years depending on Mass loss at low temperatures -NH/NHe ~1 ; Significant N-abundance -Sequences of higher mass MWD > 0.65 Msun or higher metallicity Z>0.001, DID NOT experience CNO flashes ~ ~ Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Results: Expected Lightcurves Brightening speed From ~1 to ~4 mag/yr Bolometric corrections from Flower (1996) Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Results: -Diffusion induced novas are not recurrent. Evolution during the second white dwarf stage is much faster. There is no enough time for diffusion to act. The occurrence (or not) of diffusion induced novas seems to be more complicated! -Our simulations do not follow the criterion: ΔMbuffer < ΔMH /10. For our ~0.54 Msun sequences the critical value is ΔMbuffer ~ ΔMH /5 And for our ~0.62 Msun sequences it was ΔMbuffer ~ ΔMH /30 Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Results: -Diffusion induced novas do not reduce the thickness of the H-envelope by many orders of magnitude. DAs with thin H-envelopes are not produced this way CNO-flash CNO-flash Digression (observation for asteroseismologists): Late Thermal Pulses in stars that DO experience third dredge up are a much better way of getting thin H-envelopes for DAV (Althaus et al. 2005, A&A, 440, L1) Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Differences between Diffusion induced novas and Born Again Stars Very late thermal pulses Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Differences between Diffusion induced novas and Born Again Stars -Diffusion induced novas are brighter (~2 to ~3 mag) than fast born again stars during outburst, and ~1.5 mag brighter at maximum. -Diffusion induced novas are also hotter/bluer during outburst -RCrB-like episodes after outburst???... Let’s see Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Born Again Stars experience RCrB-like events after outburst (once back on the AGB) RCrB-like RCrB-like V605 Aql V4334 Sgr But born again stars (VLTP) are very carbon rich (see Asplund et al. 1999) -RCrB-like episodes after outburstin diffusion induced novas???, I thought you needed a lot of carbon but… Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

There were RCrB-like episodes in MV Sgr A carbon deficient RCrB star (C~0.0005, N~0.0009 by mass fraction). Our diffusion induced novas have With C>O and a more Nitrogen May be Diffusion Induced Novas experience RCrB-like events after all... …If so… Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Speculation: Possible Observational Counterparts: -Very Slow Novas? (Iben & Mac Donald 1986), which takes us to… -Enigmatic object CK Vul??? (see Hajduk et al. 2007, 3 years ago in this very same room!) -Anthelms-Hevelius nova (CK Vul). Erupted between 1669 and 1670 and probably experienced RCrB like episodes before fading from view -Shara & Moffat recovered a nebula asociated with the 1669 event -Hajduk confirmed the link between the nebula and the nova And measure possible radio emission form the central object Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Speculation, Possible Observational Counterparts: CK Vul? The enigmatic Hevelius nova CK Vul escapes all present explanations. Many scenarios have been proposed to explain the object: -Very slow nova (Shara et al. 1985) -Hibernating nova (Shara et al. 1986) -Born Again Star (Harrison et al. 1996, Evans et al. 2002) -Merger of main sequence stars (Kato 2003) -”Gentle(?) Supernova”; “Light Nova”, ”Accretion Induced Born Again” (Hajduk et al. 2007) The born again scenario seems to be the best one, (Hajduk et al 2007, Evans et al. 2002) but still (very) far from the observations… -Why not a diffusion induced nova? Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Speculation, Possible Observational Counterparts: CK Vul? (Hajduk et a. 2007) D.I.N. (fast) V.L.T.P Last time experienced High Mass Loss (no old PN) 105 -106 yr ago 106 -107 yr ~104 yr (old PN?) H-abundance H-rich (probably) H-rich H-deficient RCrB-like events Yes? ? yes Luminosity ~1Lsun from UV photons assuming central object with T=70000K Equal number of UV photons if reheating with ~10000Lsun T~10000K? (within correct reheating timescale) Ejected Mass ~10-4 Msun From ~10-4 Msun to ~10-2 Msun Maximum Brightness Mv ≈ -8 (but < Mv > ≈ -6.8) Mv ≈ -5.5 Mv ≈ -4 Eruption time Rose more than two magnitudes before maximum in less than a yr 1 to 4 magnitudes per year Less than 1 magnitudes per year So neither of the scenarios correctly account for the observations but the diffusion induced nova seems to come a bit closer than the best scenario available (fast VLTP) Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Preliminary Conclusions: ●An AGB final thermal pulse or a late thermal pulse seem to provide the correct scenario to form white dwarfs with thin He-buffers. ●Diffusion induced novas DO occur in realistic white dwarf models. Together wih a thin He-buffer, low mass and metallicity seem to be necessary conditions. ●Diffusion induced novas do not produce DAs with thin H-layers as suggested by asteroseismology of some DAVs. True False The star becomes a yellow giant a few years after the CNO-flash Its surface abundance is mildly He-enriched with NH/NHe ~1 Diffusion induced novas occur when ΔMbuffer < ΔMH /10 The star luminosity brightens 10 mag, light curve look like very slow nova Diffusion induced novas are expected to be recurrent H-burning and strong winds during the giant phases will lead to H-depletion of the star, leading to the formation of non-DA white dwarfs Main Open Questions: ●How frequent do low mass stars depart from the AGB an experience an AFTP/LTP? ●Anthelme-Hevelius nova CK Vul might have been a diffusion induced nova? But before finishing the presentation… Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Don’t miss the following Posters! Asteroseismologists! Don’t miss the following Posters! New DAV chemical profiles: Evidence of differencial rotation in hot pre-white dwarfs? : Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Initial-Final Mass Relation Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Castanheira & Kepler (2009): Thin H-envelopes Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Speculation, Possible Observational Counterparts: NVS 11479 Probably a fast born again star and not a diffusion induced nova Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Speculation, Possible Observational Counterparts: NVS 11479 Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Modeling (some key points): Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Modeling (some key points): Exploring the diffusion induced nova scenario 17th European White Dwarf Workshop. Tubingen, August 16-20, 2010