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Rotation- and temperature-dependence of stellar latitudinal differential rotation
More than 600 high resolution spectra of stars with spectral type F andlater were obtained in order to search for signatures of differentialrotation in line profiles. In 147 stars the rotation law could bemeasured, with 28 of them found to be differentially rotating.Comparison to rotation laws in stars of spectral type A reveals thatdifferential rotation sets in at the convection boundary in theHR-diagram; no star that is significantly hotter than the convectionboundary exhibits the signatures of differential rotation. Four lateA-/early F-type stars close to the convection boundary and at v sin{i}≈ 100 km s-1 show extraordinarily strong absolute shear atshort rotation periods around one day. It is suggested that this is dueto their small convection zone depth and that it is connected to anarrow range in surface velocity; the four stars are very similar inTeff and v sin{i}. Detection frequencies of differentialrotation α = ΔΩ/Ω > 0 were analyzed in starswith varying temperature and rotation velocity. Measurable differentialrotation is more frequent in late-type stars and slow rotators. Thestrength of absolute shear, ΔΩ, and differential rotationα are examined as functions of the stellar effective temperatureand rotation period. The highest values of ΔΩ are found atrotation periods between two and three days. In slower rotators, thestrongest absolute shear at a given rotation rateΔΩmax is given approximately byΔΩmax ∝ P-1, i.e.,αmax ≈ const. In faster rotators, bothαmax and ΔΩmax diminish lessrapidly. A comparison with differential rotation measurements in starsof later spectral type shows that F-stars exhibit stronger shear thancooler stars do and the upper boundary in absolute shear ΔΩwith temperature is consistent with the temperature-scaling law found inDoppler Imaging measurements.
| The Geneva-Copenhagen survey of the Solar neighbourhood. Ages, metallicities, and kinematic properties of 14 000 F and G dwarfs
We present and discuss new determinations of metallicity, rotation, age,kinematics, and Galactic orbits for a complete, magnitude-limited, andkinematically unbiased sample of 16 682 nearby F and G dwarf stars. Our63 000 new, accurate radial-velocity observations for nearly 13 500stars allow identification of most of the binary stars in the sampleand, together with published uvbyβ photometry, Hipparcosparallaxes, Tycho-2 proper motions, and a few earlier radial velocities,complete the kinematic information for 14 139 stars. These high-qualityvelocity data are supplemented by effective temperatures andmetallicities newly derived from recent and/or revised calibrations. Theremaining stars either lack Hipparcos data or have fast rotation. Amajor effort has been devoted to the determination of new isochrone agesfor all stars for which this is possible. Particular attention has beengiven to a realistic treatment of statistical biases and errorestimates, as standard techniques tend to underestimate these effectsand introduce spurious features in the age distributions. Our ages agreewell with those by Edvardsson et al. (\cite{edv93}), despite severalastrophysical and computational improvements since then. We demonstrate,however, how strong observational and theoretical biases cause thedistribution of the observed ages to be very different from that of thetrue age distribution of the sample. Among the many basic relations ofthe Galactic disk that can be reinvestigated from the data presentedhere, we revisit the metallicity distribution of the G dwarfs and theage-metallicity, age-velocity, and metallicity-velocity relations of theSolar neighbourhood. Our first results confirm the lack of metal-poor Gdwarfs relative to closed-box model predictions (the ``G dwarfproblem''), the existence of radial metallicity gradients in the disk,the small change in mean metallicity of the thin disk since itsformation and the substantial scatter in metallicity at all ages, andthe continuing kinematic heating of the thin disk with an efficiencyconsistent with that expected for a combination of spiral arms and giantmolecular clouds. Distinct features in the distribution of the Vcomponent of the space motion are extended in age and metallicity,corresponding to the effects of stochastic spiral waves rather thanclassical moving groups, and may complicate the identification ofthick-disk stars from kinematic criteria. More advanced analyses of thisrich material will require careful simulations of the selection criteriafor the sample and the distribution of observational errors.Based on observations made with the Danish 1.5-m telescope at ESO, LaSilla, Chile, and with the Swiss 1-m telescope at Observatoire deHaute-Provence, France.Complete Tables 1 and 2 are only available in electronic form at the CDSvia anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or viahttp://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/418/989
| Differential rotation in rapidly rotating F-stars
We obtained high quality spectra of 135 stars of spectral types F andlater and derived ``overall'' broadening functions in selectedwavelength regions utilizing a Least Squares Deconvolution (LSD)procedure. Precision values of the projected rotational velocity v \siniwere derived from the first zero of the Fourier transformed profiles andthe shapes of the profiles were analyzed for effects of differentialrotation. The broadening profiles of 70 stars rotating faster than v\sini = 45 km s-1 show no indications of multiplicity nor ofspottedness. In those profiles we used the ratio of the first two zerosof the Fourier transform q_2/q_1 to search for deviations from rigidrotation. In the vast majority the profiles were found to be consistentwith rigid rotation. Five stars were found to have flat profilesprobably due to cool polar caps, in three stars cuspy profiles werefound. Two out of those three cases may be due to extremely rapidrotation seen pole on, only in one case (v \sini = 52 km s-1)is solar-like differential rotation the most plausible explanation forthe observed profile. These results indicate that the strength ofdifferential rotation diminishes in stars rotating as rapidly as v \sini>~ 50 km s-1.Table A.1 is only available at the CDS via anonymous ftp tocdsarc.u-strasbg.fr (130.79.125.5) or viahttp://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/412/813Based on observations collected at the European Southern Observatory, LaSilla, 69.D-0015(B).
| HIPPARCOS age-metallicity relation of the solar neighbourhood disc stars
We derive age-metallicity relations (AMRs) and orbital parameters forthe 1658 solar neighbourhood stars to which accurate distances aremeasured by the HIPPARCOS satellite. The sample stars comprise 1382 thindisc stars, 229 thick disc stars, and 47 halo stars according to theirorbital parameters. We find a considerable scatter for thin disc AMRalong the one-zone Galactic chemical evolution (GCE) model. Orbits andmetallicities of thin disc stars show now clear relation each other. Thescatter along the AMR exists even if the stars with the same orbits areselected. We examine simple extension of one-zone GCE models whichaccount for inhomogeneity in the effective yield and inhomogeneous starformation rate in the Galaxy. Both extensions of the one-zone GCE modelcannot account for the scatter in age - [Fe/H] - [Ca/Fe] relationsimultaneously. We conclude, therefore, that the scatter along the thindisc AMR is an essential feature in the formation and evolution of theGalaxy. The AMR for thick disc stars shows that the star formationterminated 8 Gyr ago in the thick disc. As already reported by Grattonet al. (\cite{Gratton_et.al.2000}) and Prochaska et al.(\cite{Prochaska_et.al.2000}), thick disc stars are more Ca-rich thanthin disc stars with the same [Fe/H]. We find that thick disc stars showa vertical abundance gradient. These three facts, the AMR, verticalgradient, and [Ca/Fe]-[Fe/H] relation, support monolithic collapseand/or accretion of satellite dwarf galaxies as likely thick discformation scenarios. Tables 2 and 3 are only available in electronicform at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5)or via http:/ /cdsweb.u-strasbg.fr/ cgi-bin/qcat?J/ A+A/394/927
| Catalogue of Apparent Diameters and Absolute Radii of Stars (CADARS) - Third edition - Comments and statistics
The Catalogue, available at the Centre de Données Stellaires deStrasbourg, consists of 13 573 records concerning the results obtainedfrom different methods for 7778 stars, reported in the literature. Thefollowing data are listed for each star: identifications, apparentmagnitude, spectral type, apparent diameter in arcsec, absolute radiusin solar units, method of determination, reference, remarks. Commentsand statistics obtained from CADARS are given. The Catalogue isavailable in electronic form at the CDS via anonymous ftp tocdsarc.u-strasbg.fr (130.79.128.5) or viahttp://cdsweb.u-strasbg.fr/cgi-bin/qcar?J/A+A/367/521
| Research Note Hipparcos photometry: The least variable stars
The data known as the Hipparcos Photometry obtained with the Hipparcossatellite have been investigated to find those stars which are leastvariable. Such stars are excellent candidates to serve as standards forphotometric systems. Their spectral types suggest in which parts of theHR diagrams stars are most constant. In some cases these values stronglyindicate that previous ground based studies claiming photometricvariability are incorrect or that the level of stellar activity haschanged. Table 2 is only available in electronic form at the CDS viaanonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or viahttp://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/367/297
| Initial Results of a Comprehensive Ultrasoft Survey of the Einstein IPC Database: Source List and Confirmation of the Selection Procedure
We have carried out a survey of the entire Einstein IPC database (atotal of 5934 sources) to select objects with strong components ofultrasoft X-ray emission (i.e., emission below 0.5 keV). The selectioncriteria are based on ratios of counts within three broad energy bands(i.e., X-ray ``colors''). A total of 516 objects have been selected,with 202 (39%) having been identified through correlations with otherdatabases. Of the currently identified objects, 45% are active galacticnuclei, 28% are stellar objects, 6% are ``normal'' galaxies and galaxyclusters, and the remaining 21% are ``nonstellar'' Galactic objects suchas cataclysmic variables, pulsars, and white dwarfs. We present adiscussion of the survey selection procedure, the list of selectedsources, and discussions of interesting objects from the aforementionedgroups. We discuss the remarkable success of our rather ``lowresolution'' method of estimating spectral shape and present plans forfollow-up studies of the as yet unidentified sources.
| The ROSAT all-sky survey catalogue of optically bright main-sequence stars and subgiant stars
We present X-ray data for all main-sequence and subgiant stars ofspectral types A, F, G, and K and luminosity classes IV and V listed inthe Bright Star Catalogue that have been detected as X-ray sources inthe ROSAT all-sky survey; several stars without luminosity class arealso included. The catalogue contains 980 entries yielding an averagedetection rate of 32 percent. In addition to count rates, sourcedetection parameters, hardness ratios, and X-ray fluxes we also listX-ray luminosities derived from Hipparcos parallaxes. The catalogue isalso available in electronic form via anonymous ftp tocdsarc.u-strasbg.fr (130.79.128.5) or viahttp://cdsweb.u-strasbg.fr/Abstract.html
| Convection, Thermal Bifurcation, and the Colors of A Stars
Broadband ultraviolet photometry from the TD-1 satellite andlow-dispersion spectra from the short wavelength camera of IUE have beenused to investigate a long-standing proposal of Bohm-Vitense that thenormal main-sequence A and early-F stars may divide into two differenttemperature sequences: (1) a high-temperature branch (and plateau)comprised of slowly rotating convective stars, and (2) a low-temperaturebranch populated by rapidly rotating radiative stars. We find noevidence from either data set to support such a claim, or to confirm theexistence of an "A-star gap" in the B-V color range 0.22 <= B-V <=0.28 due to the sudden onset of convection. We do observe, nonetheless,a large scatter in the 1800--2000 A colors of the A--F stars, whichamounts to ~0.65 mag at a given B-V color index. The scatter is notcaused by interstellar or circumstellar reddening. A convincing case canalso be made against binarity and intrinsic variability due topulsations of delta Sct origin. We find no correlation with establishedchromospheric and coronal proxies of convection, and thus nodemonstrable link to the possible onset of convection among the A--Fstars. The scatter is not instrumental. Approximately 0.4 mag of thescatter is shown to arise from individual differences in surface gravityas well as a moderate spread (factor of ~3) in heavy metal abundance andUV line blanketing. A dispersion of ~0.25 mag remains, which has noclear and obvious explanation. The most likely cause, we believe, is aresidual imprecision in our correction for the spread in metalabundances. However, the existing data do not rule out possiblecontributions from intrinsic stellar variability or from differential UVline blanketing effects owing to a dispersion in microturbulentvelocity.
| A catalog of far-ultraviolet point sources detected with the fast FAUST Telescope on ATLAS-1
We list the photometric measurements of point sources made by the FarUltraviolet Space Telescope (FAUST) when it flew on the ATLAS-1 spaceshuttle mission. The list contains 4698 Galactic and extragalacticobjects detected in 22 wide-field images of the sky. At the locationssurveyed, this catalog reaches a limiting magnitude approximately afactor of 10 fainter than the previous UV all-sky survey, TDl. Thecatalog limit is approximately 1 x 10-14 ergs A sq cm/s,although it is not complete to this level. We list for each object theposition, FUV flux, the error in flux, and where possible anidentification from catalogs of nearby stars and galaxies. Thesecatalogs include the Michigan HD (MHD) and HD, SAO, the HIPPARCOS InputCatalog, the Position and Proper Motion Catalog, the TD1 Catalog, theMcCook and Sion Catalog of white dwarfs, and the RC3 Catalog ofGalaxies. We identify 2239 FAUST sources with objects in the stellarcatalogs and 172 with galaxies in the RC3 catalog. We estimate thenumber of sources with incorrect identifications to be less than 2%.
| A method for estimating the fractional area coverage of active regions on dwarf F and G stars
The D3 (lambda 5876) and lambda 10830 lines arising fromtriplet levels in neutral helium appear in absorption in active (plage)regions on the Sun and, by implication, in the active regions onSun-like (F-early K) stars. These features either do not occur, orappear only very weakly, in the quite solar (or stellar) photosphere.Hence, these diagnostics are ideal tracers of magnetic regions outsideof cool spots. The appearance of D3 and lambda 10830 inabsorption immediately suggests that these lines can be utilized toinfer the fractional area coverage, or filling factor, of active regionon stellar surfaces if their intrinsic absorption strengths in theseregions are known. In particular, a meaningful lower limit to the activefilling factor can be deduced if the maximum absorption equivalent width(Wmax) in D3 or lambda 10830 as either appears instellar analogs of solar plages can be estimated. We develop thisapproach by constructing a grid of model chromospheres based on the VALC model of the quiet solar chromosphere. This thermal structure issuperposed on published models for F and G dwarf photospheres. We solvefor the non-LTE ionization of hydrogen to infer chromospheric electrondensities. We then perform a multilevel, non-LTE computation of thehelium triplet lines in the sequence of model chromospheres, taking intoaccount the potential effects of coronal XUV back radiation on the lineformation. We conservatively estimate that Wmax approximately= 100-150 mA for D3 in both F and G dwarfs. The implied lowerlimits to the filling factor of plagelike regions can be approximately20% among active solar-type stars. We extend this approach byinvestigating a method by which the actual filling factor can be deducedthrough a study of the joint response of D3 and lambda 10830to chromospheric nonradiative heating. We emphasize that our fillingfactor estimates indicate the area coverage at the height of formationof the helium triplet lines in the active chromosphere. Because of fieldline spreading with height, filling factors based on chromospheric linesare expected to exceed estimates based on purely photospheric lines.Finally, we discuss the relative importance of collisional andphotoionization processes in the formation of these importantdiagnostics.
| Ca II H and K Filter Photometry on the UVBY System. II. The Catalog of Observations
Abstract image available at:http://adsabs.harvard.edu/cgi-bin/nph-bib_query?1995AJ....109.2828T&db_key=AST
| Vitesses radiales. Catalogue WEB: Wilson Evans Batten. Subtittle: Radial velocities: The Wilson-Evans-Batten catalogue.
We give a common version of the two catalogues of Mean Radial Velocitiesby Wilson (1963) and Evans (1978) to which we have added the catalogueof spectroscopic binary systems (Batten et al. 1989). For each star,when possible, we give: 1) an acronym to enter SIMBAD (Set ofIdentifications Measurements and Bibliography for Astronomical Data) ofthe CDS (Centre de Donnees Astronomiques de Strasbourg). 2) the numberHIC of the HIPPARCOS catalogue (Turon 1992). 3) the CCDM number(Catalogue des Composantes des etoiles Doubles et Multiples) byDommanget & Nys (1994). For the cluster stars, a precise study hasbeen done, on the identificator numbers. Numerous remarks point out theproblems we have had to deal with.
| Optical Polarization of 1000 Stars Within 50-PARSECS from the Sun
Abstract image available at:http://adsabs.harvard.edu/cgi-bin/nph-bib_query?1993A&AS..101..551L&db_key=AST
| Magnetic activity in dwarf stars with shallow convective envelopes
The magnetic activity in dwarf stars with shallow convective envelopesis addressed by studying the C II and soft X-ray surface flux densitiesin relation to the stellar rotation velocity. The C II emission from theacoustically heated basal atmospheric component increases withincreasing T(eff) up to at least B-V about 0.25, reaching a level ofabout 8 x 10 exp 4 erg/sq cm/s for early F-type dwarf stars. Arelationship between rotation rate and level of magnetic activity isfound to extend down to at least B-V about 0.25, although the C IIemission associated with the magnetic activity at B-V = 0.25 issuppressed by a factor of about 100 as compared to stars cooler than B-Vabout 0.60 with the same rotation rate. The suppression of activity isstrongly color-dependent below B-V about 0.60, with the dynamoefficiency leveling off for cooler stars. The radiative lossesassociated with magnetic activity do not show a noticeable dependence oncolor in diagrams relating fluxes from chromosphere and corona for F-,G-, and K-type dwarf stars, suggesting comparable atmospheric structuresfor the magnetic component. The observed mean rotational velocities as afunction of spectral type are shown to be consistent with theassumptions of (1) a reduced dynamo efficiency and (2) a comparablemechanism for angular momentum loss through a stellar wind for allmagnetically active cool stars.
| The onset of chromospheric activity among the A and F stars
Results are reported from a search for an upper boundary for the onsetof main-sequence star activity based on a quest for high-temperature UVline emission in a large collection of IUE spectra. It is shown thatstrong chromospheric emission is common among early F dwarf and subgiantstars. At its brightest, the emission is equal to that of the mostactive solar-type stars and is exceeded only by that of the spotted RSCVn and BY Dra variables. It is suggested that the emission from themain-sequence stars reaches a peak near B-V = 0.28, in the vicinity ofspectral type F0 V, before it declines to lower flux levels among thelate A stars. Emission is seen in some dwarf stars as early as B-V =0.25. It is demonstrated that the C II emission of stars earlier thanthe spectral type F5 is uncorrelated with rotation. Previous findingsthat the coronal X-ray:chromospheric UV flux ratio is lower for starsearlier than spectral type F5 than for those later than F5 areconfirmed.
| Magnetic structure in cool stars. XVII - Minimum radiative losses from the outer atmosphere
The emissions in several chromospheric and transition region lines andin coronal soft X-rays are analyzed for a sample of cool stars. Thenature of the lower-limit flux densities is explored, and evidence isgiven for the possibility of a basal, nonmagnetic heating mechanismbeing responsible for these emission fluxes up to, and perhapsincluding, the upper transition region. It is argued that the excessflux density, derived by subtraction of the basal flux density from theobserved stellar flux, is the proper measure of magnetic activity. Thelevel of the basal flux density as a function of color is determined tobe 2 x 10 exp 6 erg/sq cm/s for F-type stars and 2 x 10 exp 5 erg/sqcm/s for K-type stars.
| Close binaries observed polarimetrically
Not Available
| The evolution of chromospheric activity of cool giant and subgiant stars
IUE spectra for a large sample of cool subgiant stars are examined, andevidence is found that subgiants in the mass range 1.2-1.6 solar massesundergo a sudden decline in UV transition region emission near B - V =0.6, which corresponds to spectral type G0 IV. The decline in UVemission coincides with a sharp decrease in stellar rotation rates, andit is suggested that this decay in activity and rotation marks atransformation from acoustic heating in the early F stars to magneticdynamo-driven activity in the cooler stars, resulting in a strongrotational braking action by stellar wind. For more massive giant stars,there is a similar transformation in the nature of chromosphericactivity near B - V = 0.7, or spectral type G0 III, from acousticheating in the F-type giants to a solarlike dynamo mechanism in thecooler giants. No sign of an abrupt drop in activity near spectral typeG5 III at the location of Gray's proposed rotational boundary line isseen.
| Activity in Warm Stars
Not Available
| On the reality of certain spectroscopic orbits
A review of 27 spectroscopic orbits, 25 of which were derived in aninvestigation of the degree of multiplicity found among stars of solartype, discloses that 24 of them are not supported by the data upon whichthey were based. Indeed, in at least 21 cases the evidence does not showthat the stars are binaries at all. The multiplicity of solar-type starshas therefore probably been overestimated. It is suggested that similarreviews of multiplicity among other groups of stars might lead toanalogous conclusions.
| Activity in F stars
Measurements of He I 5876 A and IUE measurements of chromospheric andtransition region lines in a large sample of F-type stars are presented.The data show that activity is detectable in nearly all early F-typestars and differs in several of its characteristics from that typicallyseen in cooler stars with slow rotation and fully developed convectivezones. The onset of activity occurs near B-V = 0.28, which correspondsapproximately to spectral type F0 and T(eff) = 7300 K. There is nocorrelation between the level of activity and the abundances of lithiumand beryllium in F stars hotter than T(eff) = 6600 K. All but one of thestars in the 6600-7300 K temperature interval are active. The levels ofactivity in these stars are independent of Rossby number.
| The dependence of He I 10830 A absorption strength upon X-ray emission in late-type stars
Measurements of He I 10830 A absorption equivalent widths and fractionalX-ray luminosities L(x)/L(bo) are presented for a large sample oflate-type stars. A correlation of increasing 10830 A strength withincreasing L(x)/L(bo) is evident in dwarfs, giants, and supergiantslater than and including spectral type F7. No equivalent correlation isapparent in main-sequence stars earlier than dF7 (B-V of about 0.5). Thedata suggest that coronal X-ray irradiation constitutes an importantsource of He I excitation in late-type stars. The fact that X-rayluminosity depends exponentially on 10830 A equivalent width isattributed to the production of X-rays in active regions covering only afraction of the stellar surface. It is conjectured that the absence of10830 A X-ray correlation in early dF stars is due to the increasedimportance of electron collisional excitation of He I. This effect isdiscussed in light of evidence that the nature of magnetic activitychanges significantly across the color range spanned by dF stars; achange related directly to the increasing depth of stellar convectionwith decreasing effective temperature.
| An Einstein Observatory X-ray survey of main-sequence stars with shallow convection zones
The results of an X-ray survey of bright late A and early F stars on themain B-V sequence between 0.1 and 0.5 are presented. All the stars wereobserved with the Einstein Observatory for a period of at least 500seconds. The survey results show significantly larger X-ray luminositiesfor the sample binaries than for the single stars. It is suggested thatthe difference is due to the presence of multiple X-ray sources inbinaries. It is shown that the X-ray luminosities for single starsincrease rapidly with increasing color, and that the relation Lx/Lbol isequal to about 10 to the -7th does not hold for A stars. No correlationwas found between X-ray luminosity and projected equatorial rotationvelocity. It is argued on the basis of the observations that X-rayemission in the sample stars originated from coronae. The availableobservational evidence supporting this view is discussed.
| Spectroscopic binaries - 14th complementary catalog
Orbital-element data for 380 spectroscopic binaries are compiled andannotated in tables. The catalog represents a continuation of the 13thcatalog (Pedoussaut and Nadal, 1977) and uses the same general format.The techniques used in making the magnitudes and spectral typeshomogeneous are indicated.
| A period-finding method for sparse randomly spaced observations of 'How long is a piece of string?'
A mathematical method for identifying the correct period of a variablestar from a small number of unequally spaced observations is presented.Previous methods using Fourier-transform and least-squares techniquesare reviewed. The true-string-length approach of Burke et al. (1970) isrefined by scaling the observations to place equal emphasis on theobservational and periodic members of the equation. It is shown that theminimum string length corresponding to a correct variable-star periodwill lie between 1.4 and 1.8. The effect of random error is considered,and criteria for predicting the number of false periods that will begenerated by the method are presented. The computational routine isdescribed. The method is demonstrated on several stars, and a new orbitis characterized for 17 Lyr, a spectroscopic binary observed by Abt andLevy (1976). An advantage of the method is seen in the fact that it canestimate the period of a variable after as few as 20 observations,allowing the timing of further observations to be planned efficiently.
| On the coronae of rapidly rotating stars. IV - Coronal activity in F dwarfs and implications for the onset of the dynamo
X-ray observations of 14 early F dwarfs are reported and these stars areused, together with a complete sample from the literature, to examinehow the characteristics of coronal X-ray emission vary from dwarfs ofspectral type A through G. Evidence for a rotation-activity relation instars redder than B - V = 0.45 is found. Stellar duplicity and age,except insofar as they influence the rotation rate, do not appear to beimportant in determining the coronal X-ray flux level in F dwarfs. It issuggested that the appearance of a relation between rotation andactivity at B - V = 0.45 indicates the turn-on of a solar-like dynamo.The high X-ray surface fluxes and small variance thereof for dwarfs withB - V = 0.3-0.45 are also discussed.
| A search for secondary lines in the visual spectra of 55 binaries
Using a CCD detector in the Kitt Peak coude spectrograph, a search wasmade for secondary lines in the visual spectral region of single-linedbinaries. The lines were found in one-quarter of the 23 B2-B5 dwarfs and6 percent of the 32 F3-G2 dwarfs. In the cases of failures, there are nocontradictions between the earliest possible secondary spectral typesand the latest types allowed by the orbital mass functions.
| Apparent radii and other parameters for 416 B5 V-F5 V stars of the catalogue of the Geneva Observatory
Apparent radius, visual brightness, effective temperature and absoluteradius for 416 B5 v-F5 v stars of the catalogue of the GenevaObservatory (Rufener, 1976) have been determined. Twenty-eight stars,anomalous in log a" versus (m~)o diagrams, have been singled out. A goodcorrelation for seven stars, in common with the list of Hanbury Brown etal. (1974), has been found. Similar parameters determined for 279 B5v-F5 v stars of two preceding papers (Fracassini et al., 1973, 1975)have allowed us to determine the averaged diagrams , and versus (B -V)0 for 695 B5 v-F5 v stars. Moreover, in the present paper a goodcorrelation versus and carefulrelation = -7.40 + 3.31 for B5v-F5 V stars have been determined. Plain correlations between log R/R0and blanketing parameter m2 for some spectral types seem to point outthat there are real differences in the absolute radii of stars of thesame spectral type, in agreement with recent researches on the HRdiagram (Houck and Fesen, 1978). Systematic differences between double(spectroscopic and visual) and single stars are found. In particular,the averaged relation versus shows that A2v-F5 v double stars may have a higher metallicity index m2 and smallerabsolute radii than single stars. Finally, the diagram log v sin iversus log R/R0 confirms some properties of binary systems found byother researchers (Huang, 1966; Plavec, 1970; Levato, 1974; Kitamura andKondo, 1978)
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Pozíciós és asztrometriai adatok
| Csillagkép: | Északi Vízikígyó |
| Rektaszcenzió: | 10h10m05.90s |
| Deklináció: | -12°48'58.0" |
| Vizuális fényesség: | 5.31 |
| Távolság: | 27.315 parszek |
| RA sajátmozgás: | -122.3 |
| Dec sajátmozgás: | -109.3 |
| B-T magnitude: | 5.712 |
| V-T magnitude: | 5.338 |
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