Exploring the diffusion induced nova scenario Marcelo Miguel Miller Bertolami Leandro Gabriel Althaus (FCAGLP-UNLP/IALP CONICET, Argentina) Exploring the.

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

Stellar Evolution. Evolution on the Main Sequence Zero-Age Main Sequence (ZAMS) MS evolution Development of an isothermal core: dT/dr = (3/4ac) (  r/T.
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.
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.
Astronomy 535 Stellar Structure Evolution. Course Philosophy “Crush them, crush them all!” -Professor John Feldmeier.
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.
Stellar Structure Section 6: Introduction to Stellar Evolution Lecture 16 – Evolution of core after S-C instability Formation of red giant Evolution up.
Lecture 15PHYS1005 – 2003/4 Lecture 16: Stellar Structure and Evolution – I Objectives: Understand energy transport in stars Examine their internal structure.
Evolved Massive Stars. Wolf-Rayet Stars Classification WNL - weak H, strong He, NIII,IV WN2-9 - He, N III,IV,V earliest types have highest excitation.
Institute for Astronomy and Astrophysics, University of Tübingen, Germany July 5, 2004Cool Stars, Stellar Systems and the Sun (Hamburg, Germany)1 Turning.
Properties of stars during hydrogen burning Hydrogen burning is first major hydrostatic burning phase of a star: Hydrostatic equilibrium: a fluid element.
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.
Age of M13: 14 billion years. Mass of stars leaving the main-sequence ~0.8 solar masses Main Sequence Sub- giants Giants Helium core- burning stars.
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.
1 The structure and evolution of stars Lecture 10: The evolution of 1M  mass stars.
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,
PHYSICS UNDER THE BONNET OF A STELLAR EVOLUTION CODE Richard J. Stancliffe Argelander Institut für Astronomie, Universität Bonn.
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.
Lecture 16 Post-ms evolution. Overview: evolution.
Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland1 Light and.
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.
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.
Chapter 11 The Death of High Mass Stars
The Future of White Dwarf Asteroseismology Travis Metcalfe (NCAR) NGC 1514 – Crystal Ball Nebula.
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
Discussion Explain why a star expands when its core collapses once it runs out of hydrogen in its core.
Stars on and off the Main Sequence
Star Formation - 6 (Chapter 5 – Universe).
Exploring the diffusion induced nova scenario
Mariko KATO (Keio Univ., Japan) collaboration with
Stellar Evolution Chapters 16, 17 & 18.
HST/COS Observations of O(He) Stars
25.2 – Stellar Evolution – Part II
How Stars Evolve Pressure and temperature The fate of the Sun
Annoucements Next test is in one week
Stellar Evolution Chapter 19.
Life Cycle of a Star Star Life Cycle: Stars are like humans. They are born, live and then die.
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
The Deaths of Stars.
ASTEROSEISMOLOGY OF LATE STAGES OF STELLAR EVOLUTION
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 17 th European White Dwarf Workshop. Tubingen, August 16-20, 2010

Exploring the diffusion induced nova scenario 17 th 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 in two different flavors: H-rich: Renedo et al. 2010, ApJ, 717, 183H-deficient: Althaus et al. 2009, ApJ, 704, 1605 See poster by Renedo et al. !

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

Exploring the diffusion induced nova scenario 17 th European White Dwarf Workshop. Tubingen, August 16-20, 2010 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 N H/ N He ~1  Diffusion induced novas occur when ΔM buffer < ΔM H /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 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 Objectives ●Diffusion induced novas might lead to very thin H-envelopes as those predicted by some asteroseismological studies of DAV (see Castanheira & Kepler 2009).

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

Exploring the diffusion induced nova scenario 17 th 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.

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 17 th European White Dwarf Workshop. Tubingen, August 16-20, 2010 Modeling (some key points): The White Dwarf phase

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

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

Exploring the diffusion induced nova scenario 17 th 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 ): years -Expansion times (  2 ): years -Reheating time: from ~50 to ~400 years depending on Mass loss at low temperatures -N H/ N He ~1 ; Significant N-abundance -Sequences of higher mass M WD > 0.65 M sun or higher metallicity Z>0.001, DID NOT experience CNO flashes ~ ~

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

Exploring the diffusion induced nova scenario 17 th 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. -Our simulations do not follow the criterion: ΔM buffer < ΔM H /10. For our ~0.54 M sun sequences the critical value is ΔM buffer ~ ΔM H /5 And for our ~0.62 M sun sequences it was ΔM buffer ~ ΔM H /30 The occurrence (or not) of diffusion induced novas seems to be more complicated!

Exploring the diffusion induced nova scenario 17 th 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 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) CNO-flash

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

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

Exploring the diffusion induced nova scenario 17 th European White Dwarf Workshop. Tubingen, August 16-20, RCrB-like episodes after outburstin diffusion induced novas???, I thought you needed a lot of carbon but… Born Again Stars experience RCrB-like events after outburst (once back on the AGB) V605 AqlV4334 Sgr RCrB-like But born again stars (VLTP) are very carbon rich (see Asplund et al. 1999)

Exploring the diffusion induced nova scenario 17 th 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~ 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 17 th 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 17 th 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 17 th European White Dwarf Workshop. Tubingen, August 16-20, 2010 Speculation, Possible Observational Counterparts: CK Vul? CK Vul (Hajduk et a. 2007) D.I.N.(fast) V.L.T.P Last time experienced High Mass Loss (no old PN) yr ago yr~10 4 yr (old PN?) H-abundanceH-rich (probably)H-richH-deficient RCrB-like eventsYes??yes Luminosity~1L sun from UV photons assuming central object with T=70000K Equal number of UV photons if reheating with ~10000L sun T~10000K? (within correct reheating timescale) Equal number of UV photons if reheating with ~10000L sun T~10000K? (within correct reheating timescale) Ejected Mass~10 -4 M sun From ~10 -4 M sun to ~10 -2 M sun Maximum Brightness M v ≈ -8 (but ≈ -6.8) M v ≈ -5.5M v ≈ -4 Eruption timeRose 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)

 The star becomes a yellow giant a few years after the CNO-flash  Its surface abundance is mildly He-enriched with N H/ N He ~1  Diffusion induced novas occur when ΔM buffer < ΔM H /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 Exploring the diffusion induced nova scenario 17 th European White Dwarf Workshop. Tubingen, August 16-20, 2010 Preliminary Conclusions: True False True False 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? ●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. But before finishing the presentation…

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

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

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

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

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

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

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