•Chemistry in Protoplanetary Disks ERIC HERBST DEPARTMENTS OF PHYSICS AND ASTRONOMY THE OHIO STATE UNIVERSITY dense (giant) molecular clouds organic molecules H core 4 -3 n = 10 cm T = 10 K 2 PDR’s embedded stars hot ionized gas HII region protoplanetary disk studied in millimeter-wave and IR CLASSIFICATIONS OF PROTOSTARS m m m GAS PHASE INTERSTELLAR/CIRCUMSTELLAR MOLECULES - HIGH RESOLUTION (9/02) _____________________________________________________________________________________________ H2 KCl HNC C3S C5 C6H HC4CN HCO NH3 CH3 H3O+ CH AlCl CH4 CH3OH AlF HCO+ H2CO SiH4 CH3SH NH PN HOC+ H2CS CH2NH C2H4 OH SiN HN2+ HCCH H2C3(lin) CH3CN C2 SiO HNO HCNH+ c-C3H2 CH3NC C7H, C6H2 C8H HCOOCH3 CH3COOH CH3C2CN H2C6(lin) C6H2 H2COHCHO C2H5OH (CH3)2O CH+ CN SiS HCS+ H2CN CH2CN HC2CHO C2H5CN CO CO+ SO+ C3 C2O CO2 C2S C3H(lin) c-C3H NH2CN CH3C4H CH2CO NH2CHO HC3NH+ HCCN HCOOH C4H2 H2C4(lin) HNCO SiC3 HOCO+ C4H HNCS C2CN C3O NaCN HCCNC HNCCC C4Si H2COH+ CSi + CP H3 CS HF NO CH2 NH2 SiC2 SiCN SO2 NS SO HCl NaCl H2O H2S C2H HCN OCS MgNC MgCN N2O HC2CN C5H C5N CH3NH2 CH2CHOH CH3CCH CH3CHO CH2CHCN c-CH2OCH2 c-CH2SCH2 HC6CN (CH2OH)2 (CH3)2CO CH3C4CN? NH2CH2COOH? HC8CN c-C6H6 HC10CN + ISOTOPOMERS Dust particles contain 1% of interstellar matter. POTENTIAL ENERGY OF REACTION activation energy typical neutral reactions radical-radical reactions some radical-stable reactions A+B ion-molecule reactions k(T) = A(T) exp(-Ea /kT) C+ D Cosmic rays produce ions “Primary” Fractionation Reaction (i) H3+ + HD H2D+ + H2 + 232 K H2D+/H3+ >> HD/H2 Signature of depletion!!! Other deuterated species GAS-PHASE MODELS A+ + B C+ + D k1 C+ + D PRODUCTS k2 d[C+]/dt = k1[A+][B] – k2[C+][D] Constraints: initial concentrations, elemental abundances, density, charge neutrality Steady-state solution: d[C+]/dt = 0 exists for constant density but takes very long (107 yr) to be achieved. CURRENT GAS-PHASE MODEL NETWORKS 4,000 reactions; 10-20% "studied"; 400 species through 13 atoms in size elements: H, He, N, O, C, S, Si, Fe, Na, Mg, P, Cl elemental abundances: “low metal” photodestruction: external, internal (via cosmic rays) Successes for quiescent cores: (1)Reproduces 80% of abundances including ions, radicals, isomers (2)Predicts strong deuterium fractionation (diffusion) TYPES OF SURFACE REACTIONS REACTANTS: MAINLY MOBILE ATOMS AND RADICALS A + B H + AB H H2 association X XH (X = O, C, N, CO, etc.) WHICH CONVERTS H + O OH H2O C CH CH2 CH3 CH4 N NH NH2 NH3 CO HCO H2CO H3CO CH3OH X + Y XY ?????????? H + HX H2 + X abstraction Diffusive Surface Chemistry Rate equations (non-discrete) Modified rate equations Stochastic approaches a) Monte Carlo b) Master equation Some Star-forming Regions quiescent cores (TMC-1; gas-grain) pre-stellar cores (L1544; gas-grain) low mass protostars (IRAS 16293-2422) protoplanetary disks (DM Tau; gas + accret./desorp.) hot cores (Orion KL; gas-grain) Protoplanetary Disk (Proplyd) Column density Cosmic rays UV X-ray midplane UV 500 AU T Tauri star – 106 yr old 0.01-0.1 M0 Keplerian rotation Temperature and Density Distribution (D’Alessio et al. 1998, 1999) A. MIDPLANE Radius (AU) n(cm-3) T (K) 1 10(14) 600 10 10(12) 50 100 10(9) 20 400 10(7) 10 Heavy species condensed onto grains Calculated Major Icy Species at 30 AU from Star (Aikawa and Herbst 1999) Cloud Disk migration inwards can be compared with solid cometary material in solar system H2O**, CO, NH3, CO2, HCN ices Deuterated species HDO, DCN Deuterium fractionation in reasonable agreement with several comets Gaseous Molecular Abundances ● Molecular Line Survey at IRAM30m telescope (Dutrey et al. 1 Abundance relative to H2 Species CO HCN CN CS H2CO HCO+ C 2H Disk(DMTau) 1.4 × 10-5 5.5 × 10 -10 3.2 × 10 -9 3.3 × 10 -10 2.0 × 10 -10 7.4 × 10 -10 1.1 × 10 -8 Cloud(TMC1) 7 × 10 -5 2 × 10 -8 3 × 10 -8 1 × 10 -8 2 × 10 -8 8 × 10 -9 8 × 10 -8 Gaseous molecular abundances in disks are different from those in clouds, typically lower, but these are averages in outer disk. Chemical Models of Gas in Outer Disk Performed by 3-4 different groups Chemistry dependent on physical model chosen and on radial and vertical distances Models start with dense cloud abundances and run for 10(6) yr at fixed physical conditions and with various sources of radiation through an inhomogeneous region. Collaborators: Aikawa, van Dishoeck, van Zadelhof Details of Models Divide outer disk into elements of space; each with density and temperature Vertical Distribution R=105AU 109 9 10 cm-3 temperature 8 8 1010 T [K] density 7 7 1010 6 10 6 10 105 105 0 20 40 60 80 densiy [cm-3] 70 70 K 60 60 50 50 40 40 30 30 20 20 R = 105 AU photodissociation 100 Z(AU) accretion Too detailed for observers Icy Molecular Layer Layer PDR Column Density 2D rad. trans previous 1Dcalc. Still, too detailed for most observations! RESULTS – COLUMN DENSITIES (cm-2) Species Theory DM Tau H2 CO CN CS CCH HCN HNC HCO+ H2CO HDO 4(21) 6 (17) 2 (13) 1(12) 8(12) 2(12) 2(12) 5(12) 4(12) 6(11) 4(21) 6(16) 1(13) 1(12) 4(13) 2(12) 9(11) 1(12) 1(12) LkCa15 2(18) 2(13) 2(13) 1(15) <5(12) 2(13) 4(14) Aikawa et al. (2002); physical model of D’Alessio; theoretical results at 373 AU and 10(6) yr Line Profile from Model Disk Line profiles are calculated using non-LTE 2D radiation code. Comparison with LkCa15 (JCMT) (Rout=400AU, incl.=60o) CO J=6-5 CO 3-2 CO 2-1 HCO+ 4-3 HCN 4-3 CN 3-2