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Accretion Processes in Star Formation

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Presentation on theme: "Accretion Processes in Star Formation"— Presentation transcript:

1 Accretion Processes in Star Formation
Based on: Accretion Processes in Star Formation Lee Hartmann Cambridge Astrophysics Series, 32 Cambridge University Press

2 ACCRETION SIGNATURES IN YSO
Matter transfered from molecular cloud to YSO. The accretion leaves distinctive signatures: . Directly, in velocity field (ex., redshifted absorption in spectra:matter is falling in . Indirectly: energy losses observed in YSO need to be compensated by external sources: Gravitational potential energy is the best candidate to supply this need Visible YSO: (Class II ,III) The emerging flux is characterized by excess over photospheric fluxes appearing in emission lines and continua . T Tauri Stars: to 2-3 Msol . Herbig Ae/Be Stars (HAeBe) : M > 1.5 Msol Ages 1-10Myr

3 Protostars (Class 0,I) Close association with molecular clouds Heavily extincted (undetectable visible/nir wavelength range) Still actively receiving mass from the cloud Powerfull outflows (CO, SiO, H2, [SII], Ha …) Hartmann 2003

4 < 1970 PROPERTIES OF YSO First spectra (photograph) of
“More evolved” YSO (II,III) First spectra (photograph) of TTS (“low-mass” YSO) < 1970

5 First spectra of Herbig Ae/Be
(“Intermediate-mass YSO) Herbig 1960

6 Observational features:
Emergin flux of visible YSO is characterized by excesses over photospheric fluxes, both in emission lines and continua. Emission lines show a wide range of conditions of formation, eg: .Forbidden lines: nH 105 cm Optical/NIR : T 104K .Permitted lines: nH 1013 cm UV lines from highly ionized species T K .v ~ 0 to ~ few x 100 km/s Continuum excess appears as: flux “veiling” in photospheric absorption lines dominates the UV and IR emissions

7 Clase 1 T Tauri spectra Standard Emission lines H, HeI, NaI, CaII
“Modern” data T Tauri spectra Clase 1 Emission lines H, HeI, NaI, CaII Absorption lines with “veiling” Late spectrum (F-M types Teff K) Balmer jump B-V no photospheric Lines with “veiling” Standard photosphere from Hartmann 1998

8 Veiling Flf / Fcf + r Fl Fc 1 + r r = Fv/ Fcf Veiling parameter
Fcl Fl Flf l Flf / Fcf + r Fl Veiling parameter Fc 1 + r r = Fv/ Fcf Fv energy excess relative to the photospheric flux (Fcf) Hartigan et al 1999

9 “Veiling” Hartigan et al 1999

10 Clase 1 photosphere from Hartmann 1998 SEDS of TTS in Taurus MC
Energy excess relative to the photospheric flux in NIR and mm (Dotted curves:SED of LkCa7, classIII with no evidence for accretion) photosphere from Hartmann 1998

11 UV excess Gullbring et al 2000

12 Colour-Colour diagrams

13 NIR excess Reddening lines Kenyon & Hartmann 1995

14 CTTS locus CTTS loci Meyer, Calvet, & Hillenbrand 1997
(Colours corrected from reddening) Meyer, Calvet, & Hillenbrand 1997

15

16 CTTS vs WTTS TTS have been classified in two types: Classical (CTTS)
Weak (WTTS) Initially, classification based on the equivalent width: for WTTS, EW(Ha) < 10 A (Herbig & Bell 1988) from Hartmann 1998 Classification represented clear physical differences: WTTS : lack NIR excess no veiling excess Narrow emission lines No forbidden lines Weaker FUV lines Comparable Lx (K-L < 0.3 for photospheric colors) K 2.25 mm; L 3.4 mm

17 CTTS vs WTTS WTTS show no indication of “veiling”.
No significant NIR excess r ratio to hot continuum to stellar continuum emission at 5700 A Hartmann 1998

18 CTTS vs WTTS Emission lines in WTTS are weaker and much narrower than CTTS CTTS


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