J/A+AS/146/103   CaII H&K to CaII IRT echelle spectra    (Montes+, 2000)

Multiwavelength optical observations of chromospherically active binary systems. III. High resolution echelle spectra from CaII H & K to CaII IRT. Montes D., Fernandez-Figueroa M.J., De Castro E., Cornide M., Latorre A., Sanz-Forcada J. <Astron. Astrophys. Suppl. Ser. 146, 103 (2000)> =2000A&AS..146..103M 2000A&AS..146..103M
ADC_Keywords: Binaries, spectroscopic ; Spectroscopy Keywords: stars: activity - stars: binaries: close - stars: binaries: spectroscopic - stars: chromospheres - stars: late-type Abstract: This is the third paper of a series aimed at studying the chromosphere of active binary systems using the information provided for several optical spectroscopic features. High resolution echelle spectra including all the optical chromospheric activity indicators from the CaII H&K to CaII IRT lines are analysed here for 16 systems. The chromospheric contribution in these lines has been determined using the spectral subtraction technique. Very broad wings have been found in the subtracted Hα profile of the very active star HU Vir. These profiles are well matched using a two-component Gaussian fit (narrow and broad) and the broad component can be interpreted as arising from microflaring. Red-shifted absorption features in the Hα line have been detected in several systems and excess emission in the blue wing of FG UMa was also detected. These features indicate that several dynamical processes, or a combination of them, may be involved. Using the E/E ratio as a diagnostic we have detected prominence-like extended material viewed off the limb in many stars of the sample, and prominences viewed against the disk at some orbital phases in the dwarfs OU Gem and BF Lyn. The He I D3 line has been detected as an absorption feature in mainly all the giants of the sample. Total filling-in of the He I D3, probably due to microflaring activity, is observed in HU Vir. Self-absorption with red asymmetry is detected in the CaII H&K lines of the giants 12 Cam, FG UMa and BM CVn. All the stars analysed show clear filled-in CaII IRT lines or even notable emission reversal. The small values of the E8542/E8498 ratio we have found indicate CaII IRT emission arises from plage-like regions. Orbital phase modulation of the chromospheric emission has been detected in some systems, in the case of HU Vir evidence of an active longitude area has been found. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file stars.dat 34 16 Star positions (from Simbad) table3.dat 71 56 Hα line measures in the observed and subtracted spectra table5.dat 66 36 Hβ line measurements in the observed and subtracted spectra table6.dat 70 35 CaII H&K and Hε lines measures in the observed and subtracted spectra table7.dat 75 58 CaII IRT lines measures in the observed and subtracted spectra -------------------------------------------------------------------------------- See also: V/76 : Chromospherically Active Binaries (Strassmeier+ 1993) J/A+A/312/221 : Excess CaII H+K emission in active binaries (Montes+, 1996) Byte-by-byte Description of file: stars.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- Name Star name 12- 13 I2 h RAh Right ascension (J2000.0) 15- 16 I2 min RAm Right ascension (J2000.0) 18- 21 F4.1 s RAs Right ascension (J2000.0) 23 A1 --- DE- Declination sign (J2000.0) 24- 25 I2 deg DEd Declination (J2000.0) 27- 28 I2 arcmin DEm Declination (J2000.0) 30- 31 I2 arcsec DEs Declination (J2000.0) -------------------------------------------------------------------------------- Byte-by-byte Description of file: table3.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- Name Name 12- 17 A6 --- Obs Telescope and observation run (G1) 19- 22 F4.2 --- phi [0/1[? Orbital phase 24 A1 --- E [HCTP] Type of emission (G2) 26- 29 F4.2 --- SH ? Relative contribution of the hot component to the total continuum 30 A1 --- --- [/] 31- 34 F4.2 --- SC ? Relative contribution of the cool component to the total continuum 36 A1 --- Halpha [AEF] Observed Hα profile: A: absorption, E: emission, F: totally filled-in by emission 38- 41 F4.2 0.1nm Wobs ? Full width at half maximum in the observed spectrum 43- 46 F4.2 --- Rc Residual intensity in the observed spectrum (Rc=Fc/Fcont) 48- 51 F4.2 0.1nm EWobs ? Equivalent width in the observed spectrum 53- 56 F4.2 0.1nm Wsub ? Full width at half maximum in the subtracted spectrum 58- 61 F4.2 --- Int ? Peak emission intensity in the subtracted spectrum 63- 66 F4.2 0.1nm EWSub Excess Hα emission equivalent width in the subtracted spectrum (1) 68- 71 F4.2 [10mW/m2/nm] logFS(Ha) Absolute flux at the stellar surface -------------------------------------------------------------------------------- Note (1): Equivalent width corrected for the contribution of each component to the total continuum -------------------------------------------------------------------------------- Byte-by-byte Description of file: table5.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- Name Name 12- 17 A6 --- Obs Telescope and observation run (G1) 19- 22 F4.2 --- phi [0/1[? Orbital phase 24 A1 --- E [HCTP] Type of emission (G2) 26- 29 F4.2 0.1nm Wobs ? Full width at half maximum in the observed spectrum 31- 34 F4.2 --- Rc Residual intensity in the observed spectrum 36- 39 F4.2 0.1nm EWobs ? Equivalent width in the observed spectrum 41- 44 F4.2 0.1nm Wsub ? Full width at half maximum in the subtracted spectrum 46- 49 F4.2 --- Int ? Peak emission intensity in the subtracted spectrum 51- 54 F4.2 0.1nm EWSub Excess Hα emission equivalent width in the subtracted spectrum (1) 56- 59 F4.2 --- EW(Ha)/EW(Hb) ? Ratio of excess emission EW in the Hα and Hβ lines 61- 65 F5.2 --- E(Ha)/E(Hb) ? Corrected ratio of excess emission (2) -------------------------------------------------------------------------------- Note (1): Equivalent width corrected for the contribution of each component to the total continuum Note (2): Ratio of excess emission with the correction: E(Ha)/E(Hb) = EW(Ha)/EW(Hb)*0.2444*2.512^(B-R) given by Hall & Ramsey (1992AJ....104.1942H 1992AJ....104.1942H) -------------------------------------------------------------------------------- Byte-by-byte Description of file: table6.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- Name Name 12- 17 A6 --- Obs Telescope and observation run (G1) 19- 22 F4.2 --- phi [0/1[? Orbital phase 24 A1 --- E [CHTPS] Type of emission (G2) 26- 29 F4.2 0.1nm EW(K)r CaII K equivalent width obtained by reconstruction of the absorption line profile 31- 34 F4.2 0.1nm EW(H)r CaII H equivalent width obtained by reconstruction of the absorption line profile 36- 39 F4.2 0.1nm EW(He)r ? Hε equivalent width obtained by reconstruction of the absorption line profile 41- 44 F4.2 0.1nm EW(K)s CaII K equivalent width using spectral subtraction technique (1) 46- 49 F4.2 0.1nm EW(H)s CaII H equivalent width using spectral subtraction technique (1) 51- 54 F4.2 0.1nm EW(He)s ? Hε equivalent width using spectral subtraction technique (1) 56- 59 F4.2 [10mW/m2/nm] logF(K) CaII K surface flux (2) 61- 64 F4.2 [10mW/m2/nm] logF(H) CaII H surface flux (2) 66- 69 F4.2 [10mW/m2/nm] logF(He) ? Hε surface flux (2) -------------------------------------------------------------------------------- Note (1): Equivalent width corrected for the contribution of each component to the total continuum Note (2): Surface flux obtained by means of the linear relationship between the absolute surface flux at 3950Å (in erg/cm2/s/Å) and the colour index (V-R) by Pasquini et al. (1988A&A...191..253P 1988A&A...191..253P). -------------------------------------------------------------------------------- Byte-by-byte Description of file: table7.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- Name Name 12- 17 A6 --- Obs Telescope and observation run (G1) 19- 22 F4.2 --- phi [0/1[? Orbital phase 24 A1 --- E [CHTPS] Type of emission (G2) 26- 29 F4.2 0.1nm EW(8498)r ? λ8498 equivalent width obtained by absorption line profile reconstruction 31- 34 F4.2 0.1nm EW(8542)r ? λ8542 equivalent width obtained by absorption line profile reconstruction 36- 39 F4.2 0.1nm EW(8662)r ? λ8662 equivalent width obtained by absorption line profile reconstruction 41- 44 F4.2 0.1nm EW(8498)s ? λ8498 equivalent width using spectral subtraction technique (1) 46- 49 F4.2 0.1nm EW(8542)s ? λ8542 equivalent width using spectral subtraction technique (1) 51- 54 F4.2 0.1nm EW(8662)s ? λ8662 equivalent width using spectral subtraction technique (1) 56- 59 F4.2 --- EW(8582)/EW(8498) ? Ratio of excess emission EW (2) 61- 64 F4.2 [10mW/m2/nm] logF(8498) ? λ8498 surface flux (3) 66- 69 F4.2 [10mW/m2/nm] logF(8542) ? λ8542 surface flux (3) 71- 74 F4.2 [10mW/m2/nm] logF(8662) ? λ8662 surface flux (3) -------------------------------------------------------------------------------- Note (1): Equivalent width corrected for the contribution of each component to the total continuum. Note (2): For the observing runs in which the λ8542 and λ8498 lines are included we also give the ratio of excess emission EW, E8542/E8498, which is also an indicator of the type of chromospheric structure that produces the observed emission. Note (3): Absolute fluxes at the stellar surface have been obtained using the calibration of Hall (1996PASP..108..313H 1996PASP..108..313H) as a function of (V-R). -------------------------------------------------------------------------------- Global notes: Note (G1): Observations: CAHA95 German Spanish Observatory, 12 June 1995 INT 99 Isaac Newton Telescope, 7-8 January 1999 McD 98 Otto Struve Telescope, 12-21 January 1998 NOT 96 Nordic Optical Telescope, 1-2 March 1996 NOT 98 Nordic Optical Telescope, 5-10 April 1998 Note (G2): Type of emission: H: emission from the hot component C: emission from the cool component T: at these phases the spectral features cannot be deblended P: emission from the primary component (for MS Ser only) S: emission from the secondary component (for MS Ser only) -------------------------------------------------------------------------------- History: From A&AS electronic version References: Montes et al., Paper I 1997A&AS..125..263M 1997A&AS..125..263M Montes et al., Paper II 1998A&A...330..155M 1998A&A...330..155M
(End) Patricia Bauer [CDS] 09-Nov-2000
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