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Departures from Axisymmetry in PNe and SN1987A. M. Bobrowsky. Axisymmetry is well known. (It forms in the last part of the superwind phase -- e.g., see poster by Speck & Dijkstra) Classifications and correlations done by: Balick 1987, 2007 (APN4) Corradi & Schwarz 1995
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Departures from Axisymmetry in PNe and SN1987A M. Bobrowsky
Axisymmetry is well known. (It forms in the last part of the superwind phase -- e.g., see poster by Speck & Dijkstra) Classifications and correlations done by: Balick 1987, 2007 (APN4) Corradi & Schwarz 1995 Manchado et al. 1996, 2000 Sahai et al. 2007 Schwarz, Corradi, & Stanghellini 1992 Shaw et al. 2001 Stanghellini et al. 1999, 2000, 2002
Classification of deviations from axisymmetry • Soker & Hadar (2002) considered several types of departure from axisymmetry • Limited mainly to departures in the equatorial plane
Cause of departure — external or internal External (e.g., interaction with the ISM) Observations: Jacoby 1981; Tweedy & Kwitter 1994, 1996;Xilouris et al. 1996; Kerber et al. 2000, 2001; Muthu, Anandarao & Pottasch 2000, Rauch et al. 2000; Martin, Xilouris & Soker 2002 Theory: Borkowski, Sarazin, & Soker 1990; Soker, Borkowski, & Sarazin 1991; Villaver, Manchado, & Garcia-Segura 2000;Villaver, Garcia-Segura, & Manchado 2003; Villaver, Garcia-Segura, & Manchado 2003; Dgani & Soker 1998; see Dgani 2000 for a review
InternalDeparture (e.g., binary companion) Observations Soker, Rappaport, & Harpaz 1998; Soker 1994, 1999 Theory: Sahai 2000; Miranda et al. 2001; Miranda, Guerrero, & Torrelles 2001
About 50% of all PNe in Soker and Hadar’s sample havelarge-scale departure (compared to a 25-30% incidence of binaries). In the present work, 58% were found to have a departure from axisymmetry.
Questions to Answer • What can we learn from the departures from axisymmetry? • Can departures be generalized to other objects?
Types of Departure • Displacement of the Central Star
IC 418 (Also see poster by Morisset & Georgiev)
Central Star Displacement in the Stingray Nebula R/R~10% Assume: age = 104 yr, mass of companion = 1 Msun, and mass of central star = 1 Msun before losing mass. --> orbital period = 7.3 104 yr Distance of central star from CM of system = 1100 AU Orbital velocity = 0.5 km s-1 --> During nebular formation, star moved 1/8 of a circle in its orbit -- approximately 45˚.
Types of Departure • Displacement of the central star
Types of Departure • Displacement of the central star • Unequal size and shape of two sides
Types of Departure • Displacement of the central star • Unequal size and shape of two sides
Types of Departure • Displacement of the central star • Unequal size and shape of two sides • Bent planetary nebulae
Types of Departure • Displacement of the central star • Unequal size and shape of two sides • Bent planetary nebulae
Types of Departure • Displacement of the central star • Unequal size and shape of two sides • Bent planetary nebulae • Different lobe structures
Why different structures? • Instabilities in outer lobes when a fast wind interacts with jets? (See poster by Akashi, Soker, & Blondin.) • Fragmentation of explosively launched clumps? (See poster by Dennis, Cunningham, Frank, Balick, & Mitran.) • Other possibilities?
SN 1987A Model Morris & Podsiadlowski 2007, Science, 315, 1103 Podsiadlowski 2007, APN4
How to explain the additional 2 km sec-1 velocity? Possibilities include: • a non-radial pulsational mode excited during the early spiral-in phase • orbital motion caused by a more distant low-mass third star in the system
Conclusions • Departures from axisymmetry are significant and measurable. • Orbital motion can give expelled mass additional velocity in the direction of orbital motion. • Prospects for the Future: Generalize to other types of objects? Possibly, but use caution!