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1. Introduction

The chromospherically active binaries are detached binary systems with cool components characterized by strong chromospheric, transition region, and coronal activity. The RS CVn systems have at least one cool evolved component whereas both components of the BY Dra binaries are main sequence stars (Fekel et al. 1986).

In this series of papers we try to study the chromosphere of this kind of extremely active stars using the information provided by several optical spectroscopic features that could be used as chromospheric activity indicators. The simultaneous observations of different lines, that are formed at different height in the chromosphere (from the region of temperature minimum to the higher chromosphere), are of special interest for stellar activity studies since they provide very useful information about this stellar region. Ideally, simultaneous observations should be performed at all wavelengths in order to develop a coherent 3-D atmosphere model. In practice, simultaneous observations of several activity indicators are rare and tend to focus on the same small number of extremely active systems.

The best way to obtain the active-chromosphere contribution to some spectral line in the chromospherically active binaries is to subtract the underlying photospheric contribution using the spectral subtraction technique (subtraction of a synthesized stellar spectrum constructed from artificially rotationally broadened, radial-velocity shifted, and weighted spectra of inactive stars chosen to match the spectral types and luminosity classes of both components of the active system under consideration).

The emissions in the Ca II H & K resonance lines are the most widely used optical indicators of chromospheric activity, since their source functions are collisionally controlled and represent an extremely important cooling mechanism. In chromospheric active binaries the subtraction of the photospheric flux in this spectral region has been recently applied using the spectral subtraction (see Montes et al. 1995c, 1996a and references therein).

The Htex2html_wrap_inline2610 line is also an important chromospheric activity indicator, but it is only in emission above the continuum in very active stars, and in less active star only a filled-in absorption line is observed. So, to infer chromospheric activity level the spectral subtraction is needed (see Montes et al. 1994; 1995a,b,d, and references therein; Lázaro & Arévalo 1997). A similar behaviour is observed in the other Balmer lines (Hall & Ramsey 1992; Montes et al. 1995d).

Recently, the spectral subtraction technique has been used in other lines as the Ca II IRT, Mg I b, Na I D1, D2, and He I D3 lines (Gunn & Doyle 1997; Gunn et al. 1997). The Ca II IRT lines are formed deeper in the atmosphere and are thus sensitive probes of the temperature minimum region. The Na I D1, D2 lines are collision dominated and are good indicators of changes in the lower chromosphere. The Mg I b triplet lines are formed in the lower chromosphere and the region of temperature minimum and they are good diagnostics of photospheric activity (Basri et al. 1989). The He I D3 line has been largely ignored as activity indicator; however it could be a valuable probe of stellar activity and the observation of this line in emission supports the detection of flare like events (Zirin 1988).

In this first paper we focus our study on the analysis of the extensively used Htex2html_wrap_inline2610 chromospheric activity indicator together with simultaneous observations of the less studied He I D3 and Na I D1, D2 spectral features in a sample of 18 northern active binary systems selected from "A Catalog of Chromospherically Active Binary Stars (second edition)" (Strassmeier et al. 1993, hereafter CABS). By using the spectral subtraction technique, we have determined the excess emission in these lines and we have computed absolute chromospheric fluxes in Htex2html_wrap_inline2610. The primary aim of this study is analyse in detail the excess Htex2html_wrap_inline2610 emission and to study the subtracted Htex2html_wrap_inline2610 line profile, especially in some extremely active stars which exhibit broad wings. Moreover, we try to understand the behaviour of the He I D3 and Na I D1, D2 lines as chromospheric activity indicators taking into account the advantage that we simultaneously know the behaviour of the chromospheric excess Htex2html_wrap_inline2610 emission in these systems. In forthcoming papers we will analyze in detail several optical spectroscopic features using echelle spectroscopy in order to determine the effects of stellar activity on spectral lines originating at different heights in the chromosphere. Another of our goals is to obtain information about the presence of extended matter (prominence-like structures) in the chromospheric active binaries using simultaneous Htex2html_wrap_inline2610 and Htex2html_wrap_inline2698 observations at near-eclipse orbital phases.

In Sect. 2 we give the details of our observations and data reduction. In Sect. 3 we describe the individual results of Htex2html_wrap_inline2610, Na I D1, D2, and He I D3 line observations of our sample. Finally in Sect. 4 we discuss our results.

 

Name

Htex2html_wrap_inline2610 line region Na I D1, D2, He I D3 line region Previous obs.

Date UT tex2html_wrap_inline2726 S/N Date UT tex2html_wrap_inline2726 S/N Htex2html_wrap_inline2610 Ca II

BD Cet

1995/09/15 00:43 0.569 330 1995/09/15 01:03 0.569 361 - 95c, 96a

AY Cet

1995/09/15 02:03 0.797 385 1995/09/15 02:20 0.797 398 - 95c, 96a

AR Psc

1995/09/13 01:48 0.373 387 1995/09/13 01:27 0.372 141 94, 95a 94, 96a
'' 1995/09/14 01:42 0.443 361 1995/09/14 02:00 0.443 369 - -
'' 1995/09/15 03:55 0.519 392 1995/09/15 04:23 0.520 399 - -
'' 1995/09/15 05:34 0.524 305 1995/09/15 05:28 0.523 359 - -

HD 12545

1995/09/15 02:59 0.401 354 1995/09/15 02:25 0.400 361 - 95c, 96a

UX Ari

1995/09/13 02:08 0.419 346 95b 95c, 96a
'' 1995/09/13 05:08 0.438 202 1995/09/13 04:52 0.437 494 - -
'' 1995/09/14 02:24 0.576 276 1995/09/14 02:09 0.574 293 - -
'' 1995/09/15 03:09 0.736 352 1995/09/15 03:32 0.739 410 - -

V711 Tau

1995/09/13 05:15 0.922 360 1995/09/13 05:36 0.927 370 94, 95a 94, 96a
'' 1995/09/14 04:19 0.261 374 1995/09/14 04:35 0.265 423 - -
'' 1995/09/14 05:35 0.280 332 1995/09/14 05:50 0.283 386 - -
'' 1995/09/15 03:50 0.606 342 1995/09/15 03:44 0.605 332 - -
'' 1995/09/15 06:11 0.641 314 1995/09/15 06:05 0.639 326 - -

V833 Tau

1995/09/13 06:13 0.762 184 1995/09/15 05:47 0.752 325 95b -
'' 1995/09/14 06:07 0.319 424 1995/09/14 05:55 0.314 417 - -
'' 1995/09/15 04:56 0.851 394 1995/09/15 05:18 0.859 322 - -

V1149 Ori

1995/09/15 06:17 0.439 311 1995/09/15 06:29 0.439 335 95b 95c, 96a

MM Her

1995/09/12 20:56 0.498 274 1995/09/12 21:31 0.501 329 94, 95a 94, 96a
'' 1995/09/13 22:06 0.630 332 1995/09/13 20:45 0.623 384 - -
'' 1995/09/14 20:09 0.745 257 1995/09/14 20:41 0.748 314 - -

V815 Her

1995/09/12 20:43 0.978 360 1995/09/12 20:21 0.970 341 94, 95a 94, 96a
'' 1995/09/13 20:15 0.520 375 1995/09/13 20:22 0.523 341 - -
'' 1995/09/14 21:24 0.099 354 1995/09/14 21:44 0.107 394 - -

BY Dra

1995/09/13 22:58 0.684 387 1995/09/13 23:15 0.686 372 - 94, 96a
'' 1995/09/14 21:56 0.839 398 1995/09/14 21:05 0.838 404 - -

V775 Her

1995/09/14 22:03 0.394 342 1995/09/14 21:53 0.392 373 94, 95a 94,96a

V478 Lyr

1995/09/14 22:14 0.953 326 1995/09/14 22:33 0.959 412 - 94, 96a

HK Lac

1995/09/12 22:56 0.067 343 1995/09/12 22:42 0.067 357 94, 95a 94, 96a
'' 1995/09/13 00:42 0.070 130 1995/09/13 00:25 0.070 193 - -
'' 1995/09/13 23:44 0.110 346 1995/09/13 23:58 0.110 343 - -
'' 1995/09/14 01:37 0.113 332 1995/09/14 01:21 0.113 264 - -
'' 1995/09/14 22:53 0.149 321 1995/09/14 23:09 0.149 339 - -
'' 1995/09/15 01:26 0.153 329 1995/09/15 01:21 0.153 358 - -

AR Lac

1995/09/12 22:16 0.405 360 1995/09/12 21:57 0.399 421 94, 95a 94, 96a
'' 1995/09/13 23:39 0.939 346 1995/09/13 23:23 0.933 415 - -
'' 1995/09/14 22:49 0.425 339 1995/09/14 22:42 0.423 407 - -

KZ And

1995/09/14 23:29 0.145 336 1995/09/14 23:51 0.150 367 - 94, 95c, 96a

KT Peg

1995/09/13 00:07 0.693 221 1995/09/13 00:13 0.694 271 - 95c, 96a
" 1995/09/15 01:19 0.024 313 1995/09/15 01:13 0.023 368 - -

II Peg

1995/09/12 23.02 0.575 300 1995/09/12 23:23 0.577 298 - -
'' 1995/09/13 00:58 0.587 138 1995/09/13 01:18 0.589 240 - -
'' 1995/09/14 00:57 0.735 265 1995/09/14 01:14 0.737 324 - -
'' 1995/09/14 03:07 0.749 315 1995/09/14 02:51 0.747 328 - -
'' 1995/09/14 05:00 0.760 266 1995/09/14 05:16 0.762 263 - -
'' 1995/09/14 23:22 0.874 318 1995/09/14 23:15 0.873 324 - -
'' 1995/09/15 01:56 0.890 332 1995/09/15 01:49 0.889 352 - -
'' 1995/09/15 04:38 0.907 298 1995/09/15 04:31 0.906 311 - -

Table 1: Htex2html_wrap_inline2610 and Na I D1, D2, He I D3 Observing log, and previous Htex2html_wrap_inline2610 and Ca II H & K observations  

94: Fernández-Figueroa et al. (1994), 95a: Montes et al. (1995a), 95b: Montes et al. (1995b), 95c: Montes et al. (1995c), 96a: Montes et al. (1996a).

 

HD

Name tex2html_wrap_inline2798 SB R d V-R tex2html_wrap_inline2806 tex2html_wrap_inline2808 Vsini
(tex2html_wrap_inline2812) (pc) (days) (days) (km s-1)

1833

BD Cet K1III 1 tex2html_wrap_inline281610 71 0.81 35.1 34.46 15
7672 AY Cet WD/G5III 1 0.012/15 66.7 0.69 56.824 77.22 4
8357 AR Psc G7V/K1IV1 2 /tex2html_wrap_inline28161.5 17 0.741 14.302261 12.245 6.5/3.51
12545 XX Tri K0III 1 tex2html_wrap_inline28168 310 [0.62] 23.9824 24.3 17
21242 UX Ari G5V/K0IV 2 0.93/tex2html_wrap_inline28164.7 50 0.70/0.54 6.43791 tex2html_wrap_inline2832Ptex2html_wrap_inline2834 6/37
22468 V711 Tau G5IV/K1IV 2 1.3/3.9 36 0.62/0.75 2.83774 2.841 13/38
283750 V833 Tau dK5e 1 tex2html_wrap_inline28160.22 16.7 0.69 1.7878 1.797 6.3
37824 V1149 Ori K1III 1 tex2html_wrap_inline281611 [164] 0.90 53.58 54.1 11
341475 MM Her G2/K0IV 2 1.58/2.83 190 [/0.64] 7.960322 7.936 10/18
166181 V815 Her G5V/[M1-2V] 1 0.93:/ 31 0.54 1.8098368 1.8 27/
234677 BY Dra K4V/K7.5V 2 1.2-1.4/ 15.6 1.10 5.975112 3.827 8.0/7.4
175742 V775 Her K0V/[K5-M2V] 1 0.85/ 24 0.80 2.879395 2.898 15/
178450 V478 Lyr G8V/[dK-dM] 1 tex2html_wrap_inline28160.9 26 0.65 2.130514 2.185 21/
209813 HK Lac F1V/K0III 1 - 150 0.75 24.4284 24.4284 /15
210334 AR Lac G2IV/K0IV 2 1.8/3.1 47 0.77 1.98322195 1.98322195 46/81
218738 KZ And dK2/dK2 2 tex2html_wrap_inline28160.74/ [tex2html_wrap_inline283223] [0.74/0.74] 3.032867 3.03 12.3/11.6
222317 KT Peg G5V/K6V 2 0.93/0.72 25 [0.54/ ] 6.20199 6.092 8/5
224085 II Peg K2-3V-IV 1 2.2 29.4 0.89 6.724183 6.718 21

1 Parameters from Fekel (1996).

Table 2: Stellar parameters  


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