Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland1 Light and.

Slides:



Advertisements
Similar presentations
Prof. D.C. Richardson Sections
Advertisements

Chapter 17 Star Stuff.
Life as a Low-mass Star Image: Eagle Nebula in 3 wavebands (Kitt Peak 0.9 m).
Chapter 17 Star Stuff Lives in the Balance Our goals for learning How does a star ’ s mass affect nuclear fusion?
Stellar Evolution. The Mass-Luminosity Relation Our goals for learning: How does a star’s mass affect nuclear fusion?
Chapter 17 Star Stuff.
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.
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.
Lithium abundance in the globular cluster M4: from the Turn-Off up to the RGB Bump Collaborators: M. Salaris (University of Liverpool, UK) L. Lovisi, F.R.
Branchings, neutron sources and poisons: evidence for stellar nucleosynthesis Maria Lugaro Astronomical Institute University of Utrecht (NL)
The Lives of Stars Chapter 12. Life on Main-Sequence Zero-Age Main Sequence (ZAMS) –main sequence location where stars are born Bottom/left edge of main.
The origin of the (lighter) elements The Late Stages of Stellar Evolution Supernova of 1604 (Kepler’s)
AGB star intershell abundances inferred from analyses of extremely hot H-deficient post-AGB stars Klaus Werner Institut für Astronomie und Astrophysik.
Institute for Astronomy and Astrophysics, University of Tübingen 13 July 2007X-ray Grating Spectroscopy Cambridge, USA 1 X-ray Photospheres Klaus Werner.
Astronomers Discover Stars With Carbon Atmospheres Released at November 21, 2007 P. Dufour, J. Liebert, G. Fontaine, N. Behara published the results in.
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.
The s-process Fe Co Ni Rb Ga Ge Zn Cu Se Br As Zr Y Sr Kr (n,  ) ()() ()() r-process p-process 63 Ni, t 1/2 =100 a 64 Cu, t 1/2 =12 h, 40 % (
Center for Stellar and Planetary Astrophysics Monash University Summary prepared by John Lattanzio Abundances in M71.
Institute for Astronomy and Astrophysics, University of Tübingen, Germany July 5, 2004Cool Stars, Stellar Systems and the Sun (Hamburg, Germany)1 Turning.
Outline  Introduction  The Life Cycles of Stars  The Creation of Elements  A History of the Milky Way  Nucleosynthesis since the Beginning of Time.
Activity #32, pages (pages were done last Friday)
Life Track After Main Sequence
Kepler Center for Astro and Particle Physics, University of Tübingen Mar 30, 2009Recent Directions in Astrophysical Quantitative Spectroscopy and Radiation.
“ Analysis and interpretation of stellar spectra and nucleosynthesis processes in evolved stars ” D. A. García-Hernández (IAC Support Astronomer) Instituto.
Non-LTE in Stars The Sun Early-type stars Other spectral types.
Element abundances in PG1159 stars Klaus Werner, Thomas Rauch, Elke Reiff University of Tübingen, Germany and Jeffrey W. Kruk Johns Hopkins University,
Presolar grains and AGB stars Maria Lugaro Sterrenkundig Instituut University of Utrecht.
Stellar Fuel, Nuclear Energy and Elements How do stars shine? E = mc 2 How did matter come into being? Big bang  stellar nucleosynthesis How did different.
Creation of the Chemical Elements By Dr. Harold Williams of Montgomery College Planetarium
Lecture 2: Formation of the chemical elements Bengt Gustafsson: Current problems in Astrophysics Ångström Laboratory, Spring 2010.
A Spectroscopic Survey of Bright DA(…) White Dwarfs Alexandros Gianninas, Pierre Bergeron Université de Montréal Jean Dupuis Canadian Space Agency Maria.
Lecture 17 Post-ms evolution II. Review Review Review.
Stellar Evolution Beyond the Main Sequence. On the Main Sequence Hydrostatic Equilibrium Hydrogen to Helium in Core All sizes of stars do this After this,
Prelim Review.
1 The structure and evolution of stars Lecture 10: The evolution of 1M  mass stars.
Element abundances of bare planetary nebula central stars and the shell burning in AGB stars Klaus Werner Institut für Astronomie und Astrophysik Universität.
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.
Study of the s-process in low mass stars of Galactic disc metallicity
Chapter 17 Star Stuff.
Yields from single AGB stars Amanda Karakas Research School of Astronomy & Astrophysics Mt Stromlo Observatory.
The Sun in the Red Giant Phase (view from the Earth!)
Institute for Astronomy and Astrophysics, University of Tübingen 16 Aug th European White Dwarf Workshop Tübingen, Germany 1 HST / COS Spectroscopy.
Massive Star Evolution overview Michael Palmer. Intro - Massive Stars Massive stars M > 8M o Many differences compared to low mass stars, ex: Lifetime.
Forschungszentrum Karlsruhe in der Helmholtz-Gemeinschaft Neutron cross sections for reading the abundance history Michael Heil Forschungszentrum Karlsruhe.
Tübingen, Hydrogen-Deficient Stars1 O(He) Stars Thomas Rauch Elke Reiff Klaus Werner Jeffrey W. Kruk Institute for Astronomy and Astrophysics.
18-19 Settembre 2006 Dottorato in Astronomia Università di Bologna.
Stellar Spectroscopy and Elemental Abundances Definitions Solar Abundances Relative Abundances Origin of Elements 1.
The Abundances of Light Neutron- Capture Elements in Planetary Nebulae Nick Sterling NASA Goddard Space Flight Center June 19, 2007 Collaborators: Harriet.
FUSE spectroscopy of cool PG1159 Stars Elke Reiff (IAAT) Klaus Werner, Thomas Rauch (IAAT) Jeff Kruk (JHU Baltimore) Lars Koesterke (University of Texas)
Tubingen, September, Optical spectroscopy of the born- again Sakurai's object in 1996 Igor Savanov Simon Jeffery Don Pollacco Denis Shulyak.
Fluorine in RCB and EHe Stars. ► RCB stars comprise a sequence of H-deficient supergiants with effective temperatures from about 3500 K, as represented.
O. Straniero, L. Piersanti (Osservatorio di Teramo, INAF) R. Gallino (Universita’ di Torino) I. Dominguez (Univerdad de Granada) Light and heavy elements.
Selected Topics in Astrophysics. Solar Model (statstar) Density Mass Luminosity Temperature Nuclear Reaction Rate Pressure.
© 2010 Pearson Education, Inc. Chapter 9 Stellar Lives and Deaths (Star Stuff)
CSI661/ASTR530 Spring, 2011 Chap. 2 An Overview of Stellar Evolution Feb. 23, 2011 Jie Zhang Copyright ©
Topics in Astronomical Spectroscopy : Evolution of Chemical Abundances based on the High Resolution Stellar Spectroscopy 2010, 1 학기 대학원 이상각 19 동
Spectroscopy and the evolution of hot subdwarf stars
Chapter 17 Star Stuff.
Stellar Evolution Pressure vs. Gravity.
Star Formation Nucleosynthesis in Stars
Hydrogen Burning (Proton-proton chain)
HST/COS Observations of O(He) Stars
How Stars Evolve Pressure and temperature The fate of the Sun
Creation of the Chemical Elements
New Trends of Physics 2005, Hokkaido University, March 1
Stellar Evolution In post-Main-Sequence evolution, what you see on the surface is not a good indicator of what is happening deep in the interior.
Chapter 3, Part2 Nuclear Chemistry CHEM 396 by Dr
Presentation transcript:

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland1 Light and heavy metal abundances in hot central stars Klaus Werner University of Tübingen, Germany Collaborators: A. Hoffmann, T. Rauch, E. Reiff, I. Traulsen (Tübingen) J.W. Kruk (JHU, USA)

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland2 Outline Results from UV spectral analysis of: Some of the hottest known hydrogen-rich central stars - New T eff and log g determinations - Abundance determinations of CNO and iron Hydrogen-deficient PG1159 (central) stars Abundance determinations of neon, fluorine, iron

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland3 Analysis of hottest H-rich CSPN Observations: HST/STIS UV-spectra of 7 central stars NGC 1360, NGC 4361, NGC 6853, NGC 7293, Abell 36, LSS 1362, LS V (= Sh2-216) Selection criteria: Extremely hot (T eff around 100,000 K) UV-bright (aimed at high resolution and high-S/N) Further observations for some of these objects: FUSE far-UV spectra new optical spectra taken at CA 3.5m, SSO 2.3m, HET 9.2m

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland4 Analysis of hottest H-rich CSPN Why UV spectroscopy? The only way to determine metal abundances. Metals are highly ionized, most metals have no spectral lines in the optical The only reliable way for precise T eff determination. Many metals show lines from at least 2 ionisation stages. Problems in the optical: - He I / He II ionisation balance not available (no He I lines) - Balmer line problem still unsolved for T eff > 100,000 K (no unique model fit to all Balmer lines possible; higher Balmer series members require higher T eff )

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland5 Example: Fixing T eff of NGC 7293 by using the lines from O IV, O V, O VI

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland6 Analysis of hottest H-rich CSPN In this way, using several CNO ions, we revised T eff previously determined from optical spectra alone. Largest correction found for NGC “Evolved” from coolest to hottest object in our sample: T eff = 82,000 → 126,000 K

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland7 Analysis of hottest H-rich CSPN Stellar masses: 0.55 – 0.65 M  Traulsen et al. (2005)

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland8 Summary of abundance analysis of hottest H-rich CSPN 5 out of 7 stars have essentially solar CNO abundances (weak 3rd dredge-up because of low mass? M f =0.65 M   M i =3 M  ) Two exceptions: LS V (=Sh2-216): CNO and He 1-2 dex subsolar T eff =93,000K log g=6.9 → gravitational settling NGC 4361 This is a halo PN (Torres-Peimbert 1990) Fe lines very weak, N is subsolar by factor 10, Si by factor 20 but: O is solar and – very surprising – C is 20* oversolar Similar to K 648, the CSPN in the globular cluster M15 (Rauch et al. 2002) Possible: 12 C dredged up from C/O core

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland9 Analysis of hottest H-rich CSPN Analysis of iron (group) lines is still on-going (Fe, Ni, Cr, Mn) Many objects display Fe V and/or Fe VI and Fe VII lines → further check of T eff possible; abundances. Example: Fit to Fe VI lines in LS V +4621

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland10 New results on H-deficient PG1159 (central) stars Recall: PG1159 stars represent the transition phase from Wolf- Rayet type central stars to non-DA white dwarfs They are extremely hot: T eff = 75,000 – 200,000 K Their atmospheres are dominated by He, C, and O: e.g. prototype PG : He=33%, C=48%, O=17% (mass fractions) H-envelope ingested and burnt after a late He-shell flash Surface chemistry = material between H and He burning shells in precursor AGB-star (intershell abundances)

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland11 Prominent born-again stars: FG Sge and Sakurai’s star

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland12 AGB star structure +CO core material (dredged up) From Lattanzio (2003) M  M 

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland13 Wolf-Rayet central stars PG1159 stars non-DA white dwarfs

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland14 FUSE spectroscopy, immediate aim: identification abundance determination of trace metals PG1159 stars enable to study composition of intershell matter; usually hidden under thick H-mantle Abundances reveal nuclear reaction chains and mixing processes in stellar interior  testing stellar evolution theory Important: intershell chemistry also affects efficiency of s-process (e.g. through 12 C abundance dredged up from C/O core) H-deficient PG1159 (central) stars

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland15 s-process in AGB stars Neutron sources are 2 reactions starting from 12 C and 22 Ne nuclei (from 3α-burning shell): 12 C(p,  ) 13 N(  + ) 13 C(α,n) 16 O protons mixed down from H envelope 22 Ne(α,n) 25 Mg  depth H-burning He-burning Lattanzio 1998 s-process in 13 C pocket

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland16 H-deficient PG1159 (central) stars FUSE spectra reveal an underabundance of iron in PG1159 stars (1-2 dex); Miksa et al. (2002) Explanation: Neutron captures completely destroy iron in the 13 C pocket Accumulation of Fe-deficient matter in the intershell after each thermal pulse (pulse-driven convection) Exhibition of this matter on surface after late He-flash

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland17 H-deficient PG1159 (central) stars FUSE spectra reveal a overabundance of neon in PG1159 stars, 2% by mass = 20 times solar (Werner et al. 2004) Explanation: 22 Ne is produced in He-burning shell by alpha captures on (CNO-cycled) 14 N 22 Ne is accumulated in intershell during thermal pulses Exhibition of Ne-enriched matter on surface after late He- flash. Model predictions: Ne=2%

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland18 Ne VII Å line in FUSE spectra detectable even at solar neon abundance level: Only possibility to identify neon in hot hydrogen-rich (i.e. “normal”) central stars. PG1159 central star Ne 20 times solar (=2%) H-rich central star Ne solar Ne VII Å. For the very first time identified in astrophysical source

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland19 H-deficient PG1159 (central) stars FUSE spectra allow for the first identification of fluorine in post- AGB stars, F is solar in some PG1159 stars, but we find a strong overabundance of fluorine in other PG1159 stars, up to 200 times solar! (Werner et al. 2005) Explanation: 19 F is produced in s-processing 13 C pocket and can be accumulated in intershell during thermal pulses Exhibition of F-enriched matter on surface after late He-flash

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland20 s-process in AGB stars Neutron sources are 2 reactions starting from 12 C and 22 Ne nuclei (from 3α-burning shell): 12 C(p,  ) 13 N(  + ) 13 C(α,n) 16 O protons mixed down from H envelope 22 Ne(α,n) 25 Mg  depth H-burning He-burning Lattanzio F production in 13 C pocket

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland21 Fluorine production Nucleosynthesis path : 14 N(α,  ) 18 F(  + ) 18 O(p,α) 15 N(α,  ) 19 F Protons are provided by 14 N(n,p) 14 C with neutrons liberated from 13 C(α,n)O N and 13 C can result from H-burning by CNO cycling, but not enough to produce significant amounts of F Additional p injection from H-envelope necessary: “partial mixing” (this also activates the usual s-process)

Institute for Astronomy and Astrophysics, University of Tübingen, Germany June 29, 2005Planetary Nebulae as Astronomical Tools, Gdansk, Poland22 First discovery of fluorine in hot post-AGB stars: F VI Å fluorine abundance in PG1159 stars up to 200 times solar