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Eta Carinae: Clues to Its Binarity Ted Gull Krister Nielsen* Mike Corcoran John Hillier Kenji Hamaguchi Stefan Ivarsson Gerd Weigelt* & AMBER Team * Lead.

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Presentation on theme: "Eta Carinae: Clues to Its Binarity Ted Gull Krister Nielsen* Mike Corcoran John Hillier Kenji Hamaguchi Stefan Ivarsson Gerd Weigelt* & AMBER Team * Lead."— Presentation transcript:

1 Eta Carinae: Clues to Its Binarity Ted Gull Krister Nielsen* Mike Corcoran John Hillier Kenji Hamaguchi Stefan Ivarsson Gerd Weigelt* & AMBER Team * Lead authors in prep

2 OUTLINE Brief background of Eta Carinae including periodicity Binarity evidence from: Weigelt D STIS spectra ‘Stellar’ Line profiles A Simple model VLTI/AMBER - first result Visualization of wind structure

3  Car In late CNO cycle -- N overproduced at expense of C, O the Great Event in 1840s -1 magnitude; bright for 20 years > 12 M o Ejected -> Homunculus another event in the 1890s ~> 0.5 M o Ejected -> Little Homunculus Luminosity~ 5x10 6 L o T e ~15,000K ==>MASS>100 M o Mass Loss Rate: ~10 -3 M o /yr Wind Velocity: 500-600 km/s Historical spectrum highly variable

4 Periodic Variability implies Binarity: Damineli (1996) noted spectroscopic 5.52-year periodicity Confirmed in X-rays, IR, visible, UV in 1998.0 Coordinated observations of 2003.5 minimum RXTE period 2024+-2 days (M. Corcoran 2005) GTO (Gull), GO and Hubble Treasury (Davidson) monitoring FUSE (fuv dropped during minimum), CHANDRA (dropped to few % during minimum), VLT/UVES + STIS (echelle disp 1175- 10300A) Much being learned about properties of ejecta Much being learned about properties of ejecta Homunculus: -513 km/s Fe I, V II, Ti II @ 760K H 2 photoexcited during max, CH, OH, NH, CH + 60K Homunculus: -513 km/s Fe I, V II, Ti II @ 760K H 2 photoexcited during max, CH, OH, NH, CH + 60K Little Homunculus: -146 km/s Fe II, Cr II @ 6400K --> 5000K minimum Little Homunculus: -146 km/s Fe II, Cr II @ 6400K --> 5000K minimum Strontium filament : Neutral emission region excited by Balmer continuum Strontium filament : Neutral emission region excited by Balmer continuum

5 B, C and D are very bright emission clumps located to NE Photoexcited by Eta A & Eta B Projected distance: 300 - 600 AU Proper motion, velocity suggest in skirt between lobes, tilted at 45 0 to skyplane  Car and Weigelt Blobs Weigelt et al 1995 RMxACSmith et al 2005 ApJ Weigelt blob excitation requires UV flux of 37,000K Companion (Eta B) Verner, Bruhweiler, Gull 2005

6 Balmer alpha changes: periastron to apastron Periastron: 1998.2 Near-Apastron: 2000.2 Red=Periastron Blue=Near-Apastron Eta Carinae Weigelt D (D) _D_D D  _D_D P Cygni Absorption not present in Weigelt D except during periastron

7 He I lines blueshifted relative to H I wind lines He I lines appear to have narrow substructure for most of period He I 7065 H I 4103

8 H I 4103, He I 7065, Fe II 5170, [N II] 5756 comparison He I 7065H I 4013

9 STIS Radial 1998.0-2004.3 Curves derived from: 9 H I Balmer, Paschen lines 4 He I: 2 singlet & 2 triplet RXTE X-ray flux H I Absorption He I Absorption Velocities

10 Geometry of Wind Interactions 15000K 500 km/s 3x10 -4 M o /yr 37000K 3000km/s 10 -5 M o /yr Gas pileup from primary wind Primary wind envelopes most of binary system, except dynamic cavity carved out by secondary wind.

11 2-D model of wind- wind Interface in orbital plane. Pittard & Corcoran: D=30 AU, e=0.9

12

13 VLTI/AMBER Weigelt et al. In prep. ~ 5 mas H I Br  He I 2 1 S - 2 1 P R= 10,000 R= 1500 R=1500

14 VLTI/AMBER IR Cont: 4 mas H I: 4-6 X centered on continuum He I emis~3X; offset? He I absor: ~4 mas R=1500

15 Apastron: March 2006 VLTI/AMBER observations: We look for Eta B in continuum ~2% flux of Eta A ~8 mas PA  135 o ; He I emission velocity components along wind-wind interface Issue: sufficient UV-plane sampling? Conclusion/ Frustration STIS observations of H I, He I, Fe II ‘wind’ lines & Weigelt blobs consistent with hot binary companion blowing cavity in primary wind and He II ionization leading to He I recombination Prediction: The Holy Grail --> Eta Car B Velocity curve does not (easily) provide mass ratio.


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