Standard

Infall in Herbig Ae/Be stars: What Na D lines tell us. / Sorelli, C.; Grinin, V. P.; Natta, A.

In: Astronomy and Astrophysics, Vol. 309, No. 1, 01.05.1996, p. 155-162.

Research output: Contribution to journalArticlepeer-review

Harvard

Sorelli, C, Grinin, VP & Natta, A 1996, 'Infall in Herbig Ae/Be stars: What Na D lines tell us', Astronomy and Astrophysics, vol. 309, no. 1, pp. 155-162.

APA

Sorelli, C., Grinin, V. P., & Natta, A. (1996). Infall in Herbig Ae/Be stars: What Na D lines tell us. Astronomy and Astrophysics, 309(1), 155-162.

Vancouver

Sorelli C, Grinin VP, Natta A. Infall in Herbig Ae/Be stars: What Na D lines tell us. Astronomy and Astrophysics. 1996 May 1;309(1):155-162.

Author

Sorelli, C. ; Grinin, V. P. ; Natta, A. / Infall in Herbig Ae/Be stars: What Na D lines tell us. In: Astronomy and Astrophysics. 1996 ; Vol. 309, No. 1. pp. 155-162.

BibTeX

@article{678a01c6b2704e3ab46b14319d16eba0,
title = "Infall in Herbig Ae/Be stars: What Na D lines tell us",
abstract = "This paper discusses the origin of the redshifted absorption components observed in the Na D lines of some Herbig Ae/Be stars. We have computed non-LTE models of the thermal and ionization structure of gas clouds of different density, column density and chemical composition, from the solar one to that typical of CI-chondrites. The redshifted absorption lines can only form in small, dense, infalling gas clumps at distances ≲ 10 R, from the star. If the gas has solar chemical composition, then the clump size must be L ∼ 1011 cm (about R(Black star sign)) and the density nH ≳ 3 × 1012 c-3. These conditions can be produced at the base of a column of gas falling into the star from a circumstellar accretion disk along magnetic lines. In this case, an accretion rate Macc ≳ 3 × 10-7 M⊙ yr-1 and a stellar magnetic field of about 600 Gauss are required. As the gas metallicity increases, less dense clouds are required to fit the Na D observations. In the extreme case of a gas cloud resulting from the evaporation of CI-chondrite meteorites, it is nH ≳ 5 × 108 cm-3, L ∼ 1011 cm. The mass of the cloud is therefore of the order of 1020 gr, and the parental body must have a radius of 20 km at least. These results show that both scenarios, i.e, magnetospheric accretion and evaporation of star-grazing planetesimal bodies, are in principle possible.",
keywords = "Circumstellar matter, Herbig Ae/Be stars, Stars: formation, Stars: pre-main sequence",
author = "C. Sorelli and Grinin, {V. P.} and A. Natta",
year = "1996",
month = may,
day = "1",
language = "English",
volume = "309",
pages = "155--162",
journal = "ASTRONOMY & ASTROPHYSICS",
issn = "0004-6361",
publisher = "EDP Sciences",
number = "1",

}

RIS

TY - JOUR

T1 - Infall in Herbig Ae/Be stars: What Na D lines tell us

AU - Sorelli, C.

AU - Grinin, V. P.

AU - Natta, A.

PY - 1996/5/1

Y1 - 1996/5/1

N2 - This paper discusses the origin of the redshifted absorption components observed in the Na D lines of some Herbig Ae/Be stars. We have computed non-LTE models of the thermal and ionization structure of gas clouds of different density, column density and chemical composition, from the solar one to that typical of CI-chondrites. The redshifted absorption lines can only form in small, dense, infalling gas clumps at distances ≲ 10 R, from the star. If the gas has solar chemical composition, then the clump size must be L ∼ 1011 cm (about R(Black star sign)) and the density nH ≳ 3 × 1012 c-3. These conditions can be produced at the base of a column of gas falling into the star from a circumstellar accretion disk along magnetic lines. In this case, an accretion rate Macc ≳ 3 × 10-7 M⊙ yr-1 and a stellar magnetic field of about 600 Gauss are required. As the gas metallicity increases, less dense clouds are required to fit the Na D observations. In the extreme case of a gas cloud resulting from the evaporation of CI-chondrite meteorites, it is nH ≳ 5 × 108 cm-3, L ∼ 1011 cm. The mass of the cloud is therefore of the order of 1020 gr, and the parental body must have a radius of 20 km at least. These results show that both scenarios, i.e, magnetospheric accretion and evaporation of star-grazing planetesimal bodies, are in principle possible.

AB - This paper discusses the origin of the redshifted absorption components observed in the Na D lines of some Herbig Ae/Be stars. We have computed non-LTE models of the thermal and ionization structure of gas clouds of different density, column density and chemical composition, from the solar one to that typical of CI-chondrites. The redshifted absorption lines can only form in small, dense, infalling gas clumps at distances ≲ 10 R, from the star. If the gas has solar chemical composition, then the clump size must be L ∼ 1011 cm (about R(Black star sign)) and the density nH ≳ 3 × 1012 c-3. These conditions can be produced at the base of a column of gas falling into the star from a circumstellar accretion disk along magnetic lines. In this case, an accretion rate Macc ≳ 3 × 10-7 M⊙ yr-1 and a stellar magnetic field of about 600 Gauss are required. As the gas metallicity increases, less dense clouds are required to fit the Na D observations. In the extreme case of a gas cloud resulting from the evaporation of CI-chondrite meteorites, it is nH ≳ 5 × 108 cm-3, L ∼ 1011 cm. The mass of the cloud is therefore of the order of 1020 gr, and the parental body must have a radius of 20 km at least. These results show that both scenarios, i.e, magnetospheric accretion and evaporation of star-grazing planetesimal bodies, are in principle possible.

KW - Circumstellar matter

KW - Herbig Ae/Be stars

KW - Stars: formation

KW - Stars: pre-main sequence

UR - http://www.scopus.com/inward/record.url?scp=3242871620&partnerID=8YFLogxK

M3 - Article

AN - SCOPUS:3242871620

VL - 309

SP - 155

EP - 162

JO - ASTRONOMY & ASTROPHYSICS

JF - ASTRONOMY & ASTROPHYSICS

SN - 0004-6361

IS - 1

ER -

ID: 126126695