2010
DOI: 10.1051/0004-6361/200810224
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Multi-wavelength observations of a giant flare on CN Leonis

Abstract: Aims. In M dwarfs, optical emission lines and continua are sensitive to changing chromospheric conditions, e.g., during flares. To study flare conditions for an observed spectrum, a comparison to synthesised spectra from model atmospheres is needed. Methods. Using the stellar atmosphere code PHOENIX, we computed a set of 41 1D NLTE parameterised chromospheric models including the photosphere and parts of the transition region. By comparison of a linear combination of the synthesised spectra and a quiescent (ob… Show more

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Cited by 23 publications
(27 citation statements)
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“…Subtracting the quiescent photospheric spectrum, we also identify emission lines from neutral K and Na which fill in the core of the photospheric absorption features. These spectra are similar to red M dwarf flare spectra (Fuhrmeister et al 2008), and are understood as the result of the increase in electron density and heating of the chromosphere (Fuhrmeister et al 2010). The much longer duration of the emission lines is not surprising, and is consistent with solar flares (Zirin 1988) and the statistics of SDSS spectra of M dwarf flares (Kruse et al 2010;Hilton et al 2010).…”
Section: Spectroscopy and Photometry Of The 2012 July 29 Flaressupporting
confidence: 73%
“…Subtracting the quiescent photospheric spectrum, we also identify emission lines from neutral K and Na which fill in the core of the photospheric absorption features. These spectra are similar to red M dwarf flare spectra (Fuhrmeister et al 2008), and are understood as the result of the increase in electron density and heating of the chromosphere (Fuhrmeister et al 2010). The much longer duration of the emission lines is not surprising, and is consistent with solar flares (Zirin 1988) and the statistics of SDSS spectra of M dwarf flares (Kruse et al 2010;Hilton et al 2010).…”
Section: Spectroscopy and Photometry Of The 2012 July 29 Flaressupporting
confidence: 73%
“…However, it cannot be explained by chromospheric models alone, which have a temperature minimum well above a temperature allowing for CO. Such studies normally use linear combinations of a photospheric (or inactive chromospheric) and an active chromospheric model and have also been used for flare A136, page 11 of 21 A&A 623, A136 (2019) modeling (Fuhrmeister et al 2010). Classically this treatment is also known as 1.5D modeling, since it tries to account for the inhomogeneity of the stellar atmospheres (Ayres et al 2006).…”
Section: Linear-combination Fitsmentioning
confidence: 99%
“…These spectra were originally computed to fit the mega-flare on CN Leo (Fuhrmeister et al 2010). The stars CN Leo and Proxima Centauri have similar photospheric properties.…”
Section: Theoretical Modelling Of the Flare With Phoenixmentioning
confidence: 99%
“…Since we use a photosphere with a lower T eff than is realistic, we should infer a too high column mass for the onset of the transition region and the temperature minimum. Details about the model construction can be found in Fuhrmeister et al (2010). In this paper, we constructed the flaring model as a linear combination of a quiescent spectrum observed directly before the flare and a flaring model spectrum.…”
Section: Theoretical Modelling Of the Flare With Phoenixmentioning
confidence: 99%