1 University of Colorado, Boulder 2 SouthWest Research Institute, Boulder 3 Keck Observatory 4 UCLA...

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Main Point: Main Point: Problem: How do grains grow from d < 100 cm (gravity un-important) to d ~ km (gravity dominated) c.f. Weidenschilling, S. J., & Cuzzi, J. N. 1993, PP3 - Grains not “sticky” - Collisions tend to fragment & bounce - Head-wind => radial drift of solids => fast growth Grain growth + sedimentation + UV-photoablation  Mass-loss from disk is metal depleted  Retained disk becomes metal-enriched Gravitational instability => planetesimals Youdin, A. N., & Shu, F. H. 2002, ApJ, 580, 494 Throop, H. B. & Bally, J, 2005, ApJ, 623, L149

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1University of Colorado, Boulder2SouthWest Research Institute, Boulder3Keck Observatory 4UCLA 5NASA, Ames

Prompt UV-InducedPrompt UV-InducedPlanetesimal Formation In Disks:Planetesimal Formation In Disks:

Proplyds to Planetesimals Proplyds to Planetesimals John BallyJohn Bally11

Henry ThroopHenry Throop22

Mark Kassis3

Mark Morris4

Ralph Shuping5

Trapezium

(L = 105 Lo

t < 105 yr )

OMC 1 Outflowt = 500 yr)

(L = 105 Lo

t << 105 yr)

NKL

OMC1-S(L = 104 Lo ,

t < 105 yr)

Hundreds of Proplyds

Main Point:Main Point:• Problem: How do grains grow from d < 100 cm (gravity un-important) to d ~ 1 - 100 km (gravity dominated) c.f. Weidenschilling, S. J., & Cuzzi, J. N. 1993, PP3

- Grains not “sticky” - Collisions tend to fragment & bounce - Head-wind => radial drift of solids => fast growth • Grain growth + sedimentation + UV-photoablation Mass-loss from disk is metal depleted Retained disk becomes metal-enriched Gravitational instability => planetesimals Youdin, A. N., & Shu, F. H. 2002, ApJ, 580, 494 Throop, H. B. & Bally, J, 2005, ApJ, 623, L149

Anatomy of a proplyd

HH 508

HST4

Microjet from a proplyd: HH 508

1Ori B: 4 low-mass companions!

(Shuping et al. 2006)

Proplyd photo-ablation flows: dM/dt ~ 10-7 Mo yr -1

HST4 (LV 6), LV 1 (Shuping et al. 2006)

Posi

tion

(mas

)

Br HeI

(Williams et al. 2005) Mdisk ~ 0.003 to 0.02 Mo

HH 514

HST 2

HH 514 micro-jet in Orion: H, [HII] (HST/STIS)

Jet

Counter Jet

HST 2

Nebular H

d253-535 in M43

UV photo-ablation of disks & planet formation:UV photo-ablation of disks & planet formation:

Smith, Bally, Licht, Walawender 05

HST 10

HST 17

HST 10, 16, 17 1” = 500 AU

Bally et al. 98

HST 16200 AU diameter

0.1 pc to O7 star0.15 pc to O9.5 star

Keck AO IR HST H-alpha

(Kassis et al. 2007)

2.12 m H2 0.63 m [OI] => Soft UV photo-heating of disk surface

Growing grains: Orion 114-426 (Throop et al. 2001)

Growing grains: Si 10 m feature (Shuping et al. 2006)

The Beehive proplyd; HH 240 irradiated jet

Bally et al. 2005

kT ~ 0.57 keV & 3.55 keV NH ~ 8 x 1020 cm-2 (soft)

NH ~ 6 x 1022 cm-2 (hard) (Kastner et al. 2005, ApJS, 160, 511)

d181-825 “Beehive” proplyd Chandra COUP

Jet Star

1280 AU

d181-825 “Beehive” proplyd X-ray absorption: NH ~ 8 x1020 cm-2

But, foreground AV ~ 1 mag !

H-alpha: ne(rI) = 2.6 x 104 cm-3

dM/dt = 2.8 x 10-7 Mo yr-1

Neutral Column: (from 50 AU, V = 3 km/s) NH(RI) = 2.2 x 1021 V3

-1 r50-1

Photo-ablation flow metal depleted!

(Kastner et al. 2005, ApJS, 160, 511)

N-Body Dense-Cluster Simulations

QuickTime™ and aSorenson Video 3 decompressorare needed to see this picture.

NBODY6 code (Aarseth 2003)

Stars:• N=1000• Mstar = 500 Mo

• Salpeter IMF• R0 = 0.5 pc• O6 star fixed at center• Gas:• Mgas = 500 o

• R0 = 0.5 pc• Dispersal timescale ~2 Myr

Throop & Bally 2007

QuickTime™ and aSorenson Video 3 decompressorare needed to see this picture.

Flux History, Typical 1 Mo Star

• Flux varies by 1000x • Peak flux approaches 107 G0.• Intense close encounters with core.• There is no `typical UV flux.’• Impulsive processing.

Grain growth + Sedimentation + UVGrain growth + Sedimentation + UV => km-sized planetesimals=> km-sized planetesimals Most stars form in clusters: A, B, O stars have strong (soft) UV

Orbits => Stochastic external UV

Self-irradiation (by accretion flows)

Massive star death: blue supergiants, SN increase soft UV dose.

UV may promote planetesimal growth!

Photo-Evaporation Triggered Instability

• Gravitational collapse of dust in disk can occur if sufficiently low gas:dust ratio (Sekiya 1997; Youdin & Shu 2002)

g / d < 10 (I.e., reduction by 10x of original

gas mass)

• PE removes gas and leaves most dust– Grain growth and settling promote this

further

• Dust disk collapse provides a rapid path to planetesimal formation, without requiring particle sticking.

Throop & Bally 2005

Sedimentation + Photo-Evaporation

Self-irradiation

Gap opened at r = GM/c2

Viscous evolution + Radial migration moves dust into gap

Large dust:gas => planetesimals

Photoevaporation Off

Photoevaporation OnPhotoevaporation On

Photoevaporation On

GI unstable region

Photoevaporation On

UV => Fast Growth of Planetesimals:UV => Fast Growth of Planetesimals:

Grain growth => Solids settle to mid-planeUV => Remove dust depleted gas => High metallicity in mid-planeGravity => Instability => 1 - 100 km planetesimals

- Fast Formation of 1 to 100 km planetesimals

Throop & Bally et al. 05

ConclusionsConclusions

• UV + grain growth + sedimentation => Gravitational instability => planetesimals

• UV irradiation is stochastic: Orbital motion of low-mass stars Evolution of massive stars (3 - 40 Myr)

MS => (blue/red) supergiant => SN

Planets born as massive stars die

The End

UV Radiation may Trigger Planetissimal Formation! UV radiation may not be hazardous for planet formation!

Throop & Bally (2005, ApJ, 623, L149) show that in evolved disks in which grains have grown and sedimented to the disk-midplane BEFORE being irradiated by an external UV source, photo-ablation can actually promote the growth of planetesimals! In a sedimented disk, the gas:dust ratio at the disk surface can be larger than in the ISM. Thus, when UV radiation heats and ablates the disk, it removes dust depleted material. This process leaves the surviving portion of the disk metal enriched. Increased metallicity and grais growth can lead to the prompt formation of kilometer-scale planetesimals by gravitational instability on a time much shorter than the radial drift time-scale for centimeter to meter-sized particles. Some indirect evidence for this process has been found in Chandra X-ray studies of Orion’s proplyds (see Kastner et al. 2005, ApJS, 160, 511). The X-ray extinction (determined from X-ray spectra) to the central stars of several of Orion’s large proplyds was fond to be considerably lower than what is inferred from the hydrogen column density to the star (derived from the measured radii of the proplyd ionization fronts). In retrospect, the fiducial UV penetration depth derived from the analysis of HST images of proplyds that was derived by Johnstone, Hollenbach, & Bally (1998, ApJ, 499, 758) also is consistent with a factor of 3 to 5 times lower dust:gas ratio than found in the generatl ISM. Thus, contrary to being hazardous, UV radiation fields may actually promote the first stages of planet formation.

NKLTrapezium

OMC1-S

(L = 105 Lo

t << 105 yr)

(L = 104 Lo ,

t < 105 yr)

(L = 105 Lo

t < 105 yr )

OMC 1 Outflow

t = 500 yr)

Orion NebulaOrion Nebula

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