1990
DOI: 10.1086/169374
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Hamilton echelle spectra of young stars. I - Optical veiling

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Cited by 167 publications
(190 citation statements)
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“…To match the science spectrum, the template is then artificially veiled to account for circumstellar disk emission and its absorption lines broadened. This is achieved by adding an excess flat continuum and by convolving the template spectrum with a Gaussian of variable width (for this technique, see also Hartigan et al 1989Hartigan et al , 1991Basri & Batalha 1990). The best fit is found by minimizing the residuals after subtraction of the veiled and broadened template from the science spectrum, over a grid of veiling and broadening values.…”
Section: Photospheric Correction Of M 29 M Spectramentioning
confidence: 99%
“…To match the science spectrum, the template is then artificially veiled to account for circumstellar disk emission and its absorption lines broadened. This is achieved by adding an excess flat continuum and by convolving the template spectrum with a Gaussian of variable width (for this technique, see also Hartigan et al 1989Hartigan et al , 1991Basri & Batalha 1990). The best fit is found by minimizing the residuals after subtraction of the veiled and broadened template from the science spectrum, over a grid of veiling and broadening values.…”
Section: Photospheric Correction Of M 29 M Spectramentioning
confidence: 99%
“…For each TTS and mainsequence template in our sample, Table 1 gives pertinent stellar information, when the star was observed, and which wavelength settings were observed. Spectral types come, in order of preference, from Basri & Batalha (1990), GHBC, VBJ, Walter et al (1994), andWebb et al (1999). Rotation periods are from Bouvier (1990) and Bouvier et al (1995).…”
Section: Observationsmentioning
confidence: 99%
“…Hot spots would be created by shocks where accreting material strikes the stellar surface. Continuum emission from a hot spot "" veils ÏÏ the stellar spectrum, reducing the residual depth of photospheric absorption lines (Basri & Bertout 1989 ;Basri & Batalha 1990 ;Hartmann & Kenyon 1990 ;Hartigan et al 1991 ;Valenti, Basri, & Johns 1993, hereafter VBJ ;Gullbring et al 1998, hereafter GHBC). Many CTTSs also have redshifted absorption components in their Balmer line proÐles, indicating the presence of infalling material relatively close to the stellar surface (Hartmann 1982 ;Basri 1988 ;Edwards et al 1994 ;Alencar & Basri 2000).…”
Section: Introductionmentioning
confidence: 99%
“…The strength of the Ha line is often characteristic of strong boundary layer emission arising at the interface of a circumstellar disk and the stellar surface. Veiling from continuum emission may be important (Basri & Batalha 1990) of the absorption features. However, the fact that the forbidden emission lines are so inconspicuous suggests that any circumstellar wind is currently quite weak even though the presence of the HH object implies the existence of a mass outflow on a larger scale.…”
Section: Spectroscopic Observationsmentioning
confidence: 99%