1996A&A...305..209H


Query : 1996A&A...305..209H

1996A&A...305..209H - Astronomy and Astrophysics, volume 305209-228 (1996/1-1)

Observation and modelling of main sequence star chromospheres. V. Ultraviolet excess emission in active M dwarfs.

HOUDEBINE E.R., MATHIOUDAKIS M., DOYLE J.G. and FOING B.H.

Abstract (from CDS):

The variation in the continuum intensity (50-5000nm) of late-type M dwarfs is investigated via two grids of model atmospheres with different temperature minima. It is shown that the (E)UV intensity is mostly dependent on the transition region pressure, although the temperature minimum also plays an important role. We also observe a significant frequency redistribution of the photospheric flux when changing the minimum temperature, and a black-body type of emission from the lower chromosphere. We examine the formation of the continuum and point out that, although some differences appear for very low or very high activity levels, in general the global picture is much alike the Sun. We show that the UV continua are very good diagnostics of cool dwarf atmospheres, from the temperature minimum to the transition region. Our calculations give a good overview of the domains where physical parameters and spectral signatures are most likely observed. We compute the UBV(RIJKL)J broad band fluxes for our models and conclude that the chromospheric contribution should be detectable in the U band and possibly also in the B band. We compare our calculations to recent high resolution observations for selected stars in a narrow spectral range ((R-I)K=0.875±0.05); we show that Hα line profiles behave as expected, with a tight correlation between the line width and equivalent width. Hα emission line stars show an excess in U-B color but not in B-V. They are also more luminous than their less active absorption line counterparts, which indicates that active dwarfs have not yet reached the main sequence and are intermediate between T Tauri stars and main sequence stars. The anomalously large proportion of active stars towards late spectral types is attributed to the very slow contraction phase for low mass stars. We calculate the fluxes in the Extreme Ultraviolet Explorer Sn/SiO band (500-740A) and show that they are compatible with observed upper limits. We further compare our results for the upper activity range to pre-main sequence models and observations. They strongly support the case for a chromospheric contribution to Hα and the blue/UV excess for those objects (T Tauris, naked T Tauris, YSOs). An important conclusion is that at high pressures, corresponding to active dMe stellar atmospheres, the chromosphere becomes a very efficient radiator at continuum wavelengths. From log(M)~-5 (column mass), radiative losses in the continuum rise exponentially and faster than in Hydrogen spectral lines because of their larger optical depths. As a consequence, HI spectral lines have a small or negligible contribution to the total HI (lines and continua) and white light radiative budget. We show that the hydrogen series dominate the radiative cooling in spectral lines (from 40% to 90%) for Hα emission line stars. The cooling in the (E)UV continuum overwhelms the total radiative budget and is much larger than that in outstanding chromospheric and transition region lines (e.g. CaII, MgII, HI Lyman and Balmer). We propose this as a possible contribution for the apparent saturation observed in some spectral lines, therefore questioning the suggestion of saturation in magnetic activity levels.

Abstract Copyright: ∼

Journal keyword(s): stars: activity - chromosphere - stars: late-type - stars: pre-main sequence

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 BD+44 4548 PM* 00 05 10.8891989003 +45 47 11.641457986   11.45   9.2   M2Ve 187 0
2 HD 1326 PM* 00 18 22.8849799680 +44 01 22.637951588   9.61 8.14 7.3   M2V 602 0
3 UCAC3 252-5243 * 00 42 47.3029516752 +35 32 57.076694592       13.23   ~ 2 0
4 V* FF And SB* 00 42 48.2495037528 +35 32 55.653574200   11.84   9.941   M1Ve+M1Ve 161 0
5 BD+61 195 PM* 01 02 38.8680626986 +62 20 42.175257431   11.439   8.7   M1.5V 285 0
6 HD 275122 PM* 03 18 07.4804602684 +38 15 07.437859473   11.75 10.280 9.821 8.2 M1.5V 122 0
7 LP 356-14 A PM* 03 24 06.4798128576 +23 47 06.121608936   12.21 10.423 10.18   M1.5V 56 0
8 LP 356-14 LM* 03 24 06.48469 +23 47 06.0741 13.04 11.913 10.422 9.438 8.298 M1+M3 79 0
9 G 221-24 ** 03 48 01.6922324912 +68 40 38.765916556   12.28 10.81 10.15   M2V+K6V 65 0
10 BD-11 916 PM* 04 37 41.8657785528 -11 02 19.972109364 13.041 11.838 10.331 9.327 8.137 M1V 171 0
11 HD 36395 PM* 05 31 27.3957852161 -03 40 38.024004501 10.626 9.443 7.968 6.996 5.913 M1.5Ve 574 0
12 V* YZ CMi PM* 07 44 40.1723046464 +03 33 08.875227574 13.761 12.831 11.225 9.958 8.263 M4.0Ve 957 0
13 NAME Proxima Centauri PM* 14 29 42.9461331854 -62 40 46.164680672 14.21 12.95 11.13 9.45 7.41 M5.5Ve 1483 0
14 BD+18 3421 PM* 17 37 53.3468417549 +18 35 30.164096453 12.315 11.109 9.577 8.599 7.525 M1.5V 257 0
15 V* BY Dra BY* 18 33 55.7720712062 +51 43 08.897780286 10.22 9.23   8.733   K4Ve+K7.5Ve 639 0
16 HD 331161 ** 19 46 23.92746 +32 01 01.4390           M0.5V+M2.5V 87 0
17 HD 197481 BY* 20 45 09.5324974119 -31 20 27.237889841   10.05 8.627 9.078 6.593 M1VeBa1 1344 0
18 BD+10 4409 * 20 55 11.1244793376 +11 15 35.391502440   11.1 9.31     M3III 19 0
19 BD+40 883 SB* 21 00 05.3890094352 +40 04 12.684002015   11.588 9.969 9.63 7.96 M2.0V+M0.5V 184 0
20 V* AX Mic PM* 21 17 15.2690680973 -38 52 02.503938581   8.06 6.68     M1V 249 0
21 V* FL Aqr SB* 22 38 45.2812778993 -20 36 51.810236490   13.08 11.49 11.22 8.77 M3.5V 148 0
22 V* FK Aqr SB* 22 38 45.5746238605 -20 37 16.087447076 11.714 10.595 9.083 8.073 6.876 M0Vep 302 0
23 HD 216899 PM* 22 56 34.8046530863 +16 33 12.355636588 11.323 10.143 8.638 7.657 6.542 M1.5V 335 0
24 BD+19 5116 ** 23 31 52.17898 +19 56 14.1505 12.737 11.749 10.165 8.982 7.446 M3.5V 469 0
25 V* BR Psc BY* 23 49 12.5250852078 +02 24 04.405476893 11.532 10.427 8.993 8.029 6.946 dM1 370 0

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