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Kinematic Properties of Planetary Nebulae with WR-type Nuclei

Kinematic Properties of Planetary Nebulae with WR-type Nuclei

Talk given at 12th Asia-Pacific Regional IAU Meeting (APRIM), Daejeon, Korea, August 2014

Ashkbiz Danehkar

August 14, 2014
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  1. Kinematical Properties of
    Kinematical Properties of
    Planetary Nebulae
    Planetary Nebulae
    with WR-type Nuclei
    with WR-type Nuclei
    Ashkbiz Danehkar (Macquarie, Australia)
    Ashkbiz Danehkar (Macquarie, Australia)
    Wolfgang Steffen (UNAM, Mexico)
    Wolfgang Steffen (UNAM, Mexico)
    Quentin Parker (Macquarie/AAO)
    Quentin Parker (Macquarie/AAO)
    12
    12th
    th Asia-Pacific Regional IAU Meeting , 19 August 2014, Daejeon, Korea
    Asia-Pacific Regional IAU Meeting , 19 August 2014, Daejeon, Korea

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  2. • Introduction to Planetary Nebulae
    Introduction to Planetary Nebulae
    • Introduction to WR-type stars
    Introduction to WR-type stars
    • Planetary Nebula Morphology
    Planetary Nebula Morphology
    • Integral Field Spectroscopy
    Integral Field Spectroscopy
    • Discussion
    Discussion
    • Summary
    Summary

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  3. Herwig 2005
    NGC 6543

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  4. Why planetary nebula important?
    • Chemistry
    –Chemical contributors to the ISM
    –Mixing processes at AGB phase
    Life Elements
    AGB Products

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  5. Why planetary nebula important?
    • Morphology
    –AGB mass-loss process
    –Transition time from AGB to PN
    –But, why most axisymmetric morphologies?

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  6. • Introduction to Planetary Nebulae
    Introduction to Planetary Nebulae
    • Introduction to WR-type stars
    Introduction to WR-type stars
    • PN Morphology
    PN Morphology
    • Integral Field Spectroscopy
    Integral Field Spectroscopy
    • Discussion
    Discussion
    • Summary
    Summary

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  7. Central Stars of Planetary Nebulae
    • Most H-rich surface abundances
    • 25% H-deficient fast expanding atmospheres
    • resembling massive Wolf-Rayet (WR) stars
    • Most Carbon-sequence of Wolf-Rayet stars
    • few Nitrogen-sequence of Wolf-Rayet stars
    • few weak emission line stars (wels), weaker emission lines.
    • some emission lines similar to PG 1159 star

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  8. Central Stars of PNe (CSPNe)
    [WCL]
    [WCL]
    [WCE]
    [WCE]
    PG1159
    PG1159
    non-DAs
    non-DAs
    Bloecker 1995
    • [WCL] late-type T
    eff
    = 20,000-80,000 K, V

    =200-1000 km/s
    • [WCE] early-type T
    eff
    = 80,000-150,000 K, V

    =1200-3500 km/s
    • [WCL] → [WCE] → PG 1159 (Werner & Herwig 2006)

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  9. • Introduction to Planetary Nebulae
    Introduction to Planetary Nebulae
    • Introduction to WR-type stars
    Introduction to WR-type stars
    • Planetary Nebula Morphology
    Planetary Nebula Morphology
    • Integral Field Spectroscopy
    Integral Field Spectroscopy
    • Discussion
    Discussion
    • Summary
    Summary

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  10. • Round (R) 22% of Galactic PNe
    PN morphology
    10
    • Elliptical (E) 49%
    • Bipolar/multi-polar/ring (B) 20%
    • point-symmetric 10%

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  11. PN morphology
    Balick et al. 1987,AJ,94,1641
    • Round, Elliptical,
    Bipolar/multipolar.
    • Some included Point-
    symmetric knots.

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  12. • Introduction to Planetary Nebulae
    Introduction to Planetary Nebulae
    • Introduction to WR-type stars
    Introduction to WR-type stars
    • Planetary Nebula Morphology
    Planetary Nebula Morphology
    • Integral Field Spectroscopy
    Integral Field Spectroscopy
    • Discussion
    Discussion
    • Summary
    Summary

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  13. Integral Field Spectroscopy
    Wide Field Spectrograph (WiFeS; Dopita 2007,2010):
    • ANU 2.3-m Telescope, Siding Spring Observatory
    • image-slicing Integral Field Unit (IFU)
    • field-of-view of 25 arcsec x 38 arcsec
    • spatial resolution element of 1.0 arcsec x 0.5 arcsec
    • spectral resolution of R ~ 7000 (about 45 km/s FWHM).
    ANU 2.3 WiFeS
    Gemini 8.1 GMOS

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  14. Integral Field Spectroscopy
    • Longslit Observation (PN Hb 4)
    • IFU Observation (PN Hb 4)
    Danehkar et al. (2014)

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  15. Integral Field Spectroscopy
    • IFU Observation (PN M3-30)
    • IFU Observation (PN IC 1297)
    Danehkar et al. (2014)

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  16. Integral Field Spectroscopy
    • Spatially-Resolved Kinematics (PN M3-30)
    • Spatially-Resolved Chemistry (PN M3-30)
    Danehkar et al. (2014)

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  17. Integral Field Spectroscopy
    • Spatially-Resolved Kinematics (PN IC 1297)
    • Spatially-Resolved Chemistry (PN IC 1297)
    Danehkar et al. (2014)

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  18. Integral Field Spectroscopy
    • Spatially-Resolved Kinematics (PN Th 2-A)
    • Spatially-Resolved Chemistry (PN Th 2-A)
    Danehkar et al. (2014);
    see Poster P2-24

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  19. Integral Field Spectroscopy
    Danehkar et al. (2014), in preparation
    • Kinematical Properties of Planetary Nebulae with WR-type Nuclei
    • Kinematic modelling using SHAPE (Steffen & Lopez 2006; Steffen et al. 2011)

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  20. • Introduction to Planetary Nebulae
    Introduction to Planetary Nebulae
    • Introduction to WR-type stars
    Introduction to WR-type stars
    • Planetary Nebula Morphology
    Planetary Nebula Morphology
    • Integral Field Spectroscopy
    Integral Field Spectroscopy
    • Discussion
    Discussion
    • Summary
    Summary

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  21. PN morphology: Problems?
    Bipolar and Elliptical Morphology
    • Generalized Interacting Stellar Winds (GISW) theory
    – Kwok et al. (1978), Kahn & West (1985)
    – Unable to predict complex axisymmetric shape
    • Rotating Stellar Winds + Strong Magnetic Fields
    – Garcıa-Segura 1997; Garcıa-Segura&Lopez 2000;
    Frank&Blackman 2004
    – single star may not supply enough angular momentum
    for complex axisymmetric PNe (Soker 2006)
    • Binary System, e.g. AGB star + white dwarf → common envelope
    – Miszalski et al. 2009; De Marco 2009; Nordhaus et al. 2010
    – nearly 30% of bipolar PNe contain post-CE binaries (Miszalski et al. 2009)
    – alignments between the nebular shells and the binary orbital inclinations (e.g.
    Mitchell et al. 2007; Jones et al. 2010, 2012; Tyndall et al. 2012; Huckvale et al.
    2013).

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  22. PN morphology: Problems?
    Binary system
    • Direct Envelope Ejection
    Outflow is predominately equatorial.
    • Dynamo Driven Ejection
    Outflow is aligned around the rotation
    axis and is magnetically collimated.
    • Disk Driven Ejection
    Shred Secondary
    Outflow is aligned with rotation axis
    Nordhaus & Blackman 2006,MNRAS,370,2004

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  23. PN morphology: Problems?
    Fast, low-ionization emission regions (FLIERs)
    • Visible in [N II] 6584 and [S II] 6724 more than
    in [O III] 5007 and Hα 6563 emission
    • in opposite pairs on the both sides of
    the central star
    • moving with velocities much larger than
    the main structure (40–200 km/s)
    • How the density and velocity structures contrast
    between the FLIERs and the main body?
    – Possiblly axisymmetric mass-loss through a Common
    Envelop and angular momentum deposition of the
    binary system (Soker 1990; Soker& Harpaz (1992;
    Nordhaus & Blackman 2006).
    – Or combination of rotating stellar winds and strong
    magnetic fields (Garcıa-Segura et al. 1999; Garcıa-
    Segura & Lopez 2000)

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  24. WR Stellar Evolution: Problems?
    • Radiation pressure is too small to remove H-rich outer layer
    • There is a gap between [WCL] and [WCE]
    • Born-again scenarios:
    – AFTP. AGB Final Thermal Pulse occurs at the end of the AGB
    – LTP. Late Thermal Pulse occurs when the star moves from the AGB phase
    towards the white dwarf.
    – VLTP. Very Late Thermal Pulse
    occurs when the star is on the
    white dwarf cooling track.
    • Alternatively, mass-loss
    to a binary companion
    • or stellar merger

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  25. • Introduction to Planetary Nebulae
    Introduction to Planetary Nebulae
    • Introduction to WR-type stars
    Introduction to WR-type stars
    • Planetary Nebula Morphology
    Planetary Nebula Morphology
    • Integral Field Spectroscopy
    Integral Field Spectroscopy
    • Discussion
    Discussion
    • Summary
    Summary

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  26. Summary
    • PN asymmetric morphology: Elliptical (49%), Bipolar(20%)
    – Generalized Interacting Stellar Winds (GISW)?
    – Rotating Stellar Winds + Strong Magnetic Fields?
    – Binary System?
    • FLIERs: point-symmetric jets on the both sides
    – Moving faster than the main shell expansion
    – Low-ionization Structures, low densities
    – Mostly in PNe with hot central stars
    • H-deficient stellar atmospheres (25% of total)
    – Born-again scenarios?
    – Binary channel?
    • Problems to solve
     Asymmetric morphology of PNe
     H-deficient atmospheres of CSPNe

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  27. Acknowledgements
    Acknowledgements
    • Travel Grant from the Astronomical Society of Australia.
    Travel Grant from the Astronomical Society of Australia.
    • IAU Travel Grant from the 12th Asia-Pacific Regional IAU
    IAU Travel Grant from the 12th Asia-Pacific Regional IAU
    Meeting.
    Meeting.
    Thank you for your attention!
    Thank you for your attention!

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  28. Planetary Nebula (PN) morphology
    HST imaging
    • Round, Elliptical,
    Bipolar/multipolar.

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