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Modelling winds of really metal-poor carbon stars: Not as expected Lars Mattsson Dark Cosmology Centre, NBI, Copenhagen Anja Andersen (Dark) Bernhard Aringer (Vienna) Kjell Eriksson (Uppsala) Susanne Hfner (Uppsala) Carbon stars Mass


  1. Modelling winds of really metal-poor carbon stars: Not as expected Lars Mattsson Dark Cosmology Centre, NBI, Copenhagen Anja Andersen (Dark) Bernhard Aringer (Vienna) Kjell Eriksson (Uppsala) Susanne Höfner (Uppsala)

  2. Carbon stars

  3. Mass loss

  4. Low metallicity Sloan et al. (2008, Science, 323, 354)

  5. Model

  6. Model Mattsson et al. 2008, A&A, 484, L5

  7. Model “Standard” model star: ● Mass: 1 M 8 ● Luminosity: log(L/L 8 ) = 3.85 (~ 7080 solar lum.) ● Surface temperature: T eff = 2800 K ● Carbon excess: log(C-O) + 12 = 8.50

  8. [Fe/H] = 0.0 3.77 10 -6 15.6 0.248

  9. [Fe/H] = -0.5 3.55 10 -6 14.0 0.229

  10. [Fe/H] = -1.0 3.17 10 -6 13.4 0.218

  11. [Fe/H] = -2.0

  12. [Fe/H] = -2.0 Ballistics!

  13. [Fe/H] = -2.0 Does a higher luminosity do the trick?

  14. [Fe/H] = -2.0 Does a higher luminosity do the trick? Nope!

  15. [Fe/H] = -2.0 Log(L/L 8 ) = 4.15

  16. [Fe/H] = -2.0 But changing the effective temperature...?

  17. [Fe/H] = -2.0 But changing the effective temperature...? Not a chance!

  18. [Fe/H] = -2.0 Mattsson et al. 2010, A&A, 509, A14

  19. Molecules Molecular opacity may change this scenario: O-enhancement: C + O → CO H + O → H 2 O, OH ?? N-enhancement: H + N → NH 3 H + N + C → HCN

  20. Conclusion and open questions ● There exist a critical metallicity below which the necessary conditions for dust nucleation cannot be met. ● O/N-enhancment may improve the conditions for nucleation, but the critical metallicity seems inevitable. ● If these stars have no dust-driven winds – how do they lose their mass? Is there another mechanism? ● Or do they not lose mass and go ka-boom as some peculiar type of Type I-ish supernovae? ● Any better ideas?!?

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