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Probing high-mass star formation through different molecules

Probing high-mass star formation through different molecules. Riccardo Cesaroni INAF - Osservatorio Astrofisico di Arcetri High-mass  >8 M O  >10 3 L O  O-B star. The recipe of (OB) star formation : infall , outflow , rotation  the role of accretion disks

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Probing high-mass star formation through different molecules

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  1. Probing high-mass star formationthrough different molecules Riccardo Cesaroni INAF - Osservatorio Astrofisico di Arcetri High-mass  >8 MO >103 LOO-B star • The recipe of (OB) star formation: infall, outflow, rotation the role of accretion disks • OB star formation: observational problems • The search for disks: tracing rotation and infall • Results: disksin B stars; for O starsALMA is needed

  2. The recipe of (OB) star formation: infall, outflow, rotation Infall of circumstellar material onto protostar Two relevant timescales: accretion:tacc = Mstar/(dM/dt)acc contraction: tKH = GMstar/RstarLstar Mstar> 6-10 MOtacc > tKH (Palla & Stahler 1993) High-mass stars reach ZAMS still accreting! Spherical symmetry  Pradiation> Pram  stars > 6-10 MOshould not form!??

  3. Rotationandoutflowmay be the solution (Yorke & Sonnhalter, Kruhmolz et al.): Rotation+ang.mom.conserv.  Disk   focuses accretion   boosts ram pressure Outflow  channels stellar photons   lowers radiation pressure • Detection of accretion disks is crucial to understand O-B star formation

  4. High-mass star observations • Problems: • IMF  high-mass stars are rare • large distance: >450 pc  a few kpc ALMA sensitivity! • formation in clusters  confusion ALMA resolution! • rapidevolution: tacc=50 MO /10-3MOyr-1=5104yr • parental environment profoundly altered • Advantage: • very luminous (cont. & line) and rich (molecules)! ALMA spectral coverage!

  5. Clump UCHII HMC (CH3CN, HCOOCH3, NH3, HNCO, C2H5CN, etc. …)

  6. disk outflow outflow The search for disks: where 0.5 pc

  7. The search for disks: what

  8. Emission line from rotating disk

  9. Absorption line from infalling envelope

  10. All line tracers must be used!

  11. Results of disk searchin B and late-O (proto)stars:2 examples

  12. IRAS 20126+4104 Cesaroni et al. Hofner et al. Moscadelli et al. Keplerian rotation: M*=7 MO Moscadelli et al. (2005)

  13. Furuya et al. (2002) Beltran et al. (2004) Beltran et al. (2005)

  14. Furuya et al. (2002) Beltran et al. (2004) Beltran et al. (2005)

  15. UC HII +dust O9.5 (20 MO) + 130 MO Furuya et al. (2002) Beltran et al. (2004) Beltran et al. (2005) Keplerian rotation around 20 MO star? ALMA needed!

  16. Mdyn= 19 MO Mdyn= 55 MO = Mstar+Mgas CH3OH masers Beltran et al. (2004,2005) Goddi et al. (in prep.)

  17. absorption UC HII outflow axis

  18. infall and rotation! (dM/dt)infall > (dM/dt)HIIquench but HII exists  infall in disk! outflow axis

  19. Goddi et al. in prep. H2O maser proper motions accretion is finished!?? ALMA needed

  20. Conclusions • Robust evidence of disksin B (proto)stars and perhaps in late O (proto)stars star formation by accretion as in low-mass stars • No disk found yetin early O (proto)stars perhapsobservational bias?perhapsother star formationmechanisms possible? Only ALMA will tell: • High sensitivity & resolution  large distances • Sub-mm lines  high-T tracers  100 AU region • Wide bandwidth  outflow, infall, and rotation tracers simultaneously

  21. infall and rotation! (dM/dt)infall > (dM/dt)HIIquench but HII exists  infall in disk! outflow axis

  22. Furuya et al. (2002) Beltran et al. (2004) Beltran et al. (2005)

  23. Disksin B stars M < 10 MO R ~ 1000 AU L ~ 104 LO (dM/dt)star ~ 10-4 MO/yr trot~ 104 yr tacc~ M/(dM/dt)star~ 105 yr tacc >> trot equilibrium, circumstellar structures Toroidsin O stars M > 100 MO R ~ 10000 AU L >> 104 LO (dM/dt)star > 10-3 MO/yr trot~ 105 yr tacc~ M/(dM/dt)star~ 104 yr tacc << trot non-equilibrium, circum-cluster structures Results of disk searchTwo types of objects found:

  24. The elusive disks in early O (proto)stars • Observational bias? For Mdisk= Mstar/2, a Keplerian disk in a 50 MO star can be detected up to: • continuum sensitivity: d < 1.7 [Mstar(MO)]0.5 ~12 kpc • line sensitivity: d < 6.2 Mstar(MO) sin2i/W2(km/s)~8 kpc • spectral + angular resolution: d < 14 Mstar(MO) sin2i/[D(’’)W2(km/s)]~19 kpc disks in all O stars should be detectable up to the galactic center

  25. Caveats!!! One should consider also: • rarity of O stars  ALMA sensitivity • confusion with envelope ALMA resolution • Chemistry ALMA spectral coverage • confusion with outflow/infall ALMA resol. • non-keplerian rotation • disk flaring • inclination angle • …

  26. infall and rotation! (dM/dt)infall > (dM/dt)HIIquench but HII exists  infall in disk! outflow axis

  27. Lstar = 103-105 LO • Tdust = 65 K (Lstar/105LO)0.2 (R/0.1pc)0.4 • Tdust > 100 K for R < 0.1 pc • Grain mantles evaporated • chemical enrichment of gas phase: hot cores • wide choice of molecular probes: CH3OH, CH3CN, HCOOCH3, etc. … Jets/outflows  shocks: H2O, SiO, HCO+, etc. …

  28. Clump UCHII HMC Core

  29. IRAS 20126+4104 Edris et al. (2005) Sridharan et al. (2005) NIR & OH masers disk

  30. G192.16-3.82 Shepherd & Kurtz (1999) 2.6mm cont. disk CO outflow

  31. G192.16-3.82 Shepherd & Kurtz (1999) Shepherd et al. (2001) 3.6cm cont. & H2O masers

  32. Simon et al. (2000): TTau stars Velocity maps (CO J=21)

  33. Patel et al. (2005) Cep A HW2 Torrelles et al. (1998) … but see Comito & Schilke for a different interpretation

  34. IRAS 18089-1732 Beuther et al. (2004, 2005)

  35. Gibb et al. (2002) Olmi et al. (2003) Olmi et al. (1996) Furuya et al. (2002) Beltran et al. (2004)

  36. CH3CN(12-11) Gibb et al. (2002) Olmi et al. (2003) Beltran et al. (2005)

  37. Disks &Toroids B stars O stars

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