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Page 1: Molecular Hydrogen Emission from Protoplanetary Disks

Molecular Hydrogen Emission

from Protoplanetary

DisksHideko Nomura (Kobe Univ.), Tom Millar (UMIST)

Modeling the structure, chemistry and appearance of protoplanetary disks

Page 2: Molecular Hydrogen Emission from Protoplanetary Disks

§1 Introduction

Page 3: Molecular Hydrogen Emission from Protoplanetary Disks

106yr 107yr

Obs. of Protoplanetary Disks

SED of TTS + disk

(Chiang & Goldreich 1997)

CentralStar

Disk

StarDisk

(Andre et al. 1994)

CTTS WTTS

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Observations of H2 Line Emission

NIR GG Tau, TW Hya, LkCa 15, DoAr25 (v,J)=(1,3)-(0,1) by NOAO (Bary et al. 2003)

MIR GG Tau, GO Tau, LkCa 15 J=2-0, J=3-1 by ISO (Thi et al. 2001)

UV TW Hya 146 Lyman-band H2 lines by HST, FUSE (Herczeg et al. 2002)                etc.

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H2 Transition Lines UV pumping

UV fluorescentline emission

Infraredquandrapolar

cascades

v=0

UVpumping

continuousfluorescenc

e(UV)H+H

radiativecascade (IR)

collisionalexcitation,

de-excitation

(Shull & Beckwith 1982)

UV radiation fieldTemperature

profile

Collisional process level populations

Page 6: Molecular Hydrogen Emission from Protoplanetary Disks

Irradiation from central star

H2 level transitions via UV

pumpingHeat gas & dust

in disks

Irradiation from Central Star

(Chiang & Goldreich 1997)

CentralStar

Disk

Radiative transfer process Global physical disk structure (gas & dust temperature, and density profiles) H2 level populations & line emission

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§2 Disk Model

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Gas Density & TemperatureHydrostatic equilibrium in z-direction

zρΩρgdz

dρc 2

z2s

z

xcs

2=2kT/mp

(x)=1.4x10-7 s-1(x/1AU)-3/2 (M*=0.5 Ms )Macc=10-8Ms/yr (=const.)

Thermal equilibrium (pe+Lgr-line=0) pe : Grain photoelectric heating by FUV line :Cooling by OI, CII & CO line excitation Lgr : Energy exchange by collisions between gas and dust particles

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Dust TemperatureLocal radiative equi. (abs.=reemission)

0 grνν0 νν )(TB κdν4dΩI κdν

2D radiative transfer equationShort characteristic

method in spherical coordinate(Dullemond & Turoulla 2000)

Heating sources:(A) viscous heating at equatorial plane(B) radiation from central star

Page 10: Molecular Hydrogen Emission from Protoplanetary Disks

Stellar blackbody(T*=4000K)

+ Thermal bremsstrahlung

(Tbr=2.5 x 104K)

UV Radiation from Central Star

UV excess

(Costa et al. 2000)

TW Hya

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Resulting Temperature Profile

R=0.1AU

1AU

10AU

with UV excess without UV excessR=0.1AU

1AU

10AU

Disk surface   heated up by photoelectric heatingMidplane & Outer disk (without UV excess)    gas temp. = dust temp.

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§3 H2 Level Populations

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H2 Level PopulationsStatistical Equilibrium

lform,lm s

smlmlml2m

ldiss,lm s

slmlm2l

n(H)Rn(s)CβA)(Hn

Rn(s)Cβ)(Hn

u, B1u+ , C1u

m, X1g+

l, X1g+

UVlm

UV ml

Aml CmlClm

H+HRdiss,l

H+H

Rform,lEm>El

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Resulting Level Populations

R=0.1AU

10AU

with UV excess without UV excess

with UV excess or Inner disk (hot) : LTE collisional process, nupper: largeOuter disk without UV excess (cold) : non-LTE UV pump. & cascade, nupper: small

R=0.1AU

10AUv=0v=1 v=2 v=3v=4

v=0 v=1 v=2 v=3 v=4

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v=1-0 S(1) (@2.12m) Obs.(Bary et al.’03) with UVe without UVe (1.0 - 15) x 10-15 9.3 x 10-15 3.3 x 10-18

ObserverIul

Sul

§4 Resulting H2 Line Emission

IR

)S(Iαdz

dIululul

ul 4π

hνΦAn

α

1S ul

ululuul

ul

[erg/cm-2/s]

e.g., v=1-7 R(3) (@1489.6A) Obs.(Herczeg with with UVe without et al.’02) UVe + LyUVe 4.8 x 10-14 1.4 x 10-14 1.3 x 10-16 4.0 x 10-22

UV with UV excess:UV: nu: Iul:

with UV excess:Tgas: nu: Iul:

[erg/cm-2/s]

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§5 Discussion

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Dustless Disk ModelPlanet formation

Dustless disk model

ISgas

dust small4

gas

dust small

n

n10

n

n

Dustless disk :no infrared excess

Conserv. of dust mass& dust size growth

amount of small dust

SED

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Resulting Temperature Profile

R=0.1AU

1AU

10AU

R=0.1AU

1AU

10AU

Dusty Dustless

Dustless (ndust/ngas: small)   grain photoelectric heating Tgas

with UV excess

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Resulting Level Populations

R=0.1AU

10AUv=0v=1 v=2 v=3v=4

Dusty Dustlesswith UV excess

Outer region of dustless disk (cold) : non-LTE UV pump. & cascadenupper: large UV radiation fields dust absorption

R=0.1AU

10AU

v=0v=1 v=2 v=3 v=4

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Resulting H2 Line Emission

v=1-0 S(1) (@2.12m): Obs.(Bary et al.’03) Dusty Dustless (1.0 - 15) x 10-15 9.3 x 10-15 6.5 x 10-16

S(0) (@28.2m), S(1) (@17.0m): Obs.(Thi et al.’01) Dusty Dustless S(0) (2.5 – 5.7) x 10-14 4.2 x 10-17 9.3 x 10-17

S(1) (2.8 – 8.1) x 10-14 8.5 x 10-16 5.0 x 10-16

UV (@900A-2900A) Obs.(Herczeg et al.’02) Dusty Dustless (1.2 - 73) x 10-15 3.8 x 10-15 1.2 x 10-14

[erg/cm-2/s]

Obs. possibility to detect H2 emission from dustless disks in NIR

& UV

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§6 SummaryUV excess + Radiative transfer processGas & dust temperature, density profiles

Gas temperature@disk surface: ~2,000K Grain photoelectric heating

H2 level populations : LTE, nupper: large

Strong NIR H2 lines : consistent with obs. collisional excitation (hot gas) Strong UV H2 lines : consistent with obs. pumping by Ly emission

H2 emission from dustless disks

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