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06Nov2006 Ge/Ay133 How are disks dissipated?

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Page 1: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

06Nov2006Ge/Ay133

How are disks dissipated?

Page 2: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 3: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

Hollenbach 2006, Cambridge Disks Meeting

Page 4: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

Early disk evolution (infall from envelope):

Page 5: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

Intermediate disk evolution (pre-main sequence):

Page 6: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 7: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 8: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 9: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 10: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 11: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 12: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 13: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

The Radial & Vertical Chemical Structure of Disks

X-rays

R=300 AU

Page 14: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

To clear the inner disk,

Chemistry can have a large influence on the thermal structure:

Jonkheid et al. (2004) UV field critical…

Page 15: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

Dominated by Ly α and other lines! This has a large impact on the chemistry (CO, OH, CN, etc. do not photolyze at Ly α).

What does the VUV spectrum of a T Tauri star look like?

Heavy/Light lines = BP Tau/TW Hya

Bergin et al. (2003)

Page 16: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 17: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 18: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 19: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 20: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 21: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

External Photoevaporation scenario:

Orion Proplyd

Page 22: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

Local resonances canpropagate globally!

External Photoevaporation – Now SURFACE AREA Driven (Rapidly Shrinks)

Page 23: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 24: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 25: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 26: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 27: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 28: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 29: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 30: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

Hollenbach et al. (2000, PP IV)

Putting it all together:A comparison of various disk dispersal mechanisms

The stellar encounter (SE) and external photo-evaporation time scales are calculated for the core of the Orion proto-stellar cluster.

Page 31: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

What are the dominant processes at various disk radii?

Page 32: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

VI. What are some of the implications?

Page 33: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 34: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 35: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 36: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 37: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 38: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 39: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 40: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 41: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 42: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 43: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 44: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation
Page 45: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

Local resonances canpropagate globally!

Page 46: PowerPoint Presentation...0.1 New disc evolution model Alexander et al. (2006b) 42 -1 Evolution of surface density: ME 1M Q=IO s 10 100 1 000 ' New model incorporates direct photoevaporation

Linbladresonanceequations: