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Statistical Constraints for Astrometric Binaries with Nonlinear Motion
Useful constraints on the orbits and mass ratios of astrometric binariesin the Hipparcos catalog are derived from the measured proper motiondifferences of Hipparcos and Tycho-2 (Δμ), accelerations ofproper motions (μ˙), and second derivatives of proper motions(μ̈). It is shown how, in some cases, statistical bounds can beestimated for the masses of the secondary components. Two catalogs ofastrometric binaries are generated, one of binaries with significantproper motion differences and the other of binaries with significantaccelerations of their proper motions. Mathematical relations betweenthe astrometric observables Δμ, μ˙, and μ̈ andthe orbital elements are derived in the appendices. We find a remarkabledifference between the distribution of spectral types of stars withlarge accelerations but small proper motion differences and that ofstars with large proper motion differences but insignificantaccelerations. The spectral type distribution for the former sample ofbinaries is the same as the general distribution of all stars in theHipparcos catalog, whereas the latter sample is clearly dominated bysolar-type stars, with an obvious dearth of blue stars. We point outthat the latter set includes mostly binaries with long periods (longerthan about 6 yr).
| B Star Rotational Velocities in h and χ Persei: A Probe of Initial Conditions during the Star Formation Epoch?
Projected rotational velocities (vsini) have been measured for 216 B0-B9stars in the rich, dense h and χ Persei double cluster and comparedwith the distribution of rotational velocities for a sample of fieldstars having comparable ages (t~12-15 Myr) and masses (M~4-15Msolar). For stars that are relatively little evolved fromtheir initial locations on the zero-age main sequence (ZAMS) (those withmasses M~4-5 Msolar), the mean vsini measured for the h andχ Per sample is slightly more than 2 times larger than the meandetermined for field stars of comparable mass, and the cluster and fieldvsini distributions differ with a high degree of significance. Forsomewhat more evolved stars with masses in the range 5-9Msolar, the mean vsini in h and χ Per is 1.5 times thatof the field; the vsini distributions differ as well, but with a lowerdegree of statistical significance. For stars that have evolvedsignificantly from the ZAMS and are approaching the hydrogen exhaustionphase (those with masses in the range 9-15 Msolar), thecluster and field star means and distributions are only slightlydifferent. We argue that both the higher rotation rates and the patternof rotation speeds as a function of mass that differentiatemain-sequence B stars in h and χ Per from their field analogs werelikely imprinted during the star formation process rather than a resultof angular momentum evolution over the 12-15 Myr cluster lifetime. Wespeculate that these differences may reflect the effects of the higheraccretion rates that theory suggests are characteristic of regions thatgive birth to dense clusters, namely, (1) higher initial rotationspeeds; (2) higher initial radii along the stellar birth line, resultingin greater spin-up between the birth line and the ZAMS; and (3) a morepronounced maximum in the birth line radius-mass relationship thatresults in differentially greater spin-up for stars that become mid- tolate-B stars on the ZAMS.
| The Ca II infrared triplet as indicator of anomalous Ca isotopic mixture in HgMn stars
For the first time we present observational evidence for an anomalousisotopic structure of Ca II in mercury-manganese (HgMn) stars. Thecentroid wavelengths of Ca II infrared triplet lines in a number ofstars have been found redshifted with respect to the centroids of theterrestrial Ca II lines. The record holder is the star HD 175640 forwhich the measured wavelength is consistent with Ca II being present inthe atmosphere entirely in form of the heaviest stable isotope48Ca. This is a very striking result as 48Ca makesup only 0.187% of the terrestrial Ca mixture.Based on observations obtained at the European Southern Observator, LaSilla and Paranal, Chile (ESO programme Nos. 65.L-0316 and 67.D-0579).
| Vertical distribution of chromium in the atmospheres of HgMn stars
We use multiplet 30 Cr II lines in the wings of Hbeta totest the hypothesis of an anomalous concentration of Cr in the upperlayers of the atmospheres of a sample of 10 HgMn stars. These lines areat different distances from the H_beta line center and are thereforeformed at different depths in the stellar atmosphere. Except for HD49606, all HgMn stars show an increase in Cr abundance with height inthe stellar atmosphere. A similar vertical distribution of Cr, but lesspronounced, has been previously found in Am stars. In contrast, novariation of Cr abundance with the depth has been found for the normallate B-type star HD 196426 and the weak magnetic late B-type star HD168733. It is possible that in HgMn stars the vertical stratificationparameter, a, depends on T_eff, with the strongest vertical gradientbeing found in the hotter stars. No correlation was found between a andthe average stellar abundance log varepsilon (Cr/H).Based on observations obtained at the European Southern Observatory, LaSilla and Paranal, Chile (ESO programmes Nos. 62.L-0348, 65.I-0644,67.D-0579).
| On the elemental abundance and isotopic mixture of mercury in HgMn stars
Optical region spectra of 31 HgMn stars have been studied for theabundance and isotope mixture of mercury. In the course of theinvestigation the lines Hg I lambda 4358 and Hg Ii lambda lambda3984,6149 have been studied, with abundances established for all threelines in several HgMn stars. The mercury isotope mixture has beendetermined from high resolution spectra of the lambda 3984 line.Possible signs of an ionization anomaly have been detected by thecomparison of the abundance derived from the Hg I line and the Hg Iilines in seven of the observed HgMn stars. A possible correlation of themercury abundance with Teff has been detected. Possible signsof a weak anticorrelation of the manganese and mercury abundance in HgMnstars have been found, which could be interpreted as a sign ofinhomogeneous surface distribution of these elements. For a number ofthe HgMn stars in this study the mercury abundance and isotope mixtureare reported for the first time.
| On the relationship between the mercury-manganese stars and the metallic-lined stars
An HR diagram indicating the positions of the HgMn and the Am starsanalyzed by the senior author and his collaborators shows that thecoolest HgMn stars and the hottest Am stars are found on the samestellar evolutionary tracks and hence the former must evolve into thelater. The explanation of the dividing line between these two types ofnonmagnetic chemically peculiar stars where the Hg abundances suddenlychange their degree of overabundance is a major test of the theorieswhich try to explain the anomalous abundances of such stars. Some otherimportant relationships are found which can also serve as tests oftheories which purport to explain the properties of these stars.
| Radiative accelerations on Ne in the atmospheres of late B stars
Radiative accelerations on Ne are calculated for the atmospheres ofmain-sequence stars with 11 000 <=Teff<= 15 000 K. Thisrange corresponds to that of the mercury-manganese (HgMn) stars. Thecalculations take into account neon fine structure as well as shadowingof neon lines using the entire Kurucz line list, bound-bound, bound-freeand free-free opacity of H, He and C as well as some non-LTE effects.Non-LTE effects are found to modify the radiative acceleration by afactor of the order of 102 in the outer atmosphere and arecrucial for d m < 10-3 g cm-2. The dependenceof the radiative accelerations on the Ne abundance, effectivetemperature and gravity is studied. Radiative accelerations are found tobe well below the gravitational acceleration over the entire range ofTeff and it is predicted that in stable atmospheres devoid ofdisturbing motions, Ne should sink and be observed as under-abundant.This agrees with recent observations of low Ne abundances in HgMn stars.
| Rotational Velocities of B Stars
We measured the projected rotational velocities of 1092 northern B starslisted in the Bright Star Catalogue (BSC) and calibrated them againstthe 1975 Slettebak et al. system. We found that the published values ofB dwarfs in the BSC average 27% higher than those standards. Only 0.3%of the stars have rotational velocities in excess of two-thirds of thebreakup velocities, and the mean velocity is only 25% of breakup,implying that impending breakup is not a significant factor in reducingrotational velocities. For the B8-B9.5 III-V stars the bimodaldistribution in V can be explained by a set of slowly rotating Ap starsand a set of rapidly rotating normal stars. For the B0-B5 III-V starsthat include very few peculiar stars, the distributions in V are notbimodal. Are the low rotational velocities of B stars due to theoccurrence of frequent low-mass companions, planets, or disks? Therotational velocities of giants originating from late B dwarfs areconsistent with their conservation of angular momentum in shells.However, we are puzzled by why the giants that originate from the earlyB dwarfs, despite having 3 times greater radii, have nearly the samerotational velocities. We find that all B-type primaries in binarieswith periods less than 2.4 days have synchronized rotational and orbitalmotions; those with periods between 2.4 and 5.0 days are rotating withina factor 2 of synchronization or are ``nearly synchronized.'' Thecorresponding period ranges for A-type stars are 4.9 and 10.5 days, ortwice as large. We found that the rotational velocities of the primariesare synchronized earlier than their orbits are circularized. The maximumorbital period for circularized B binaries is 1.5 days and for Abinaries is 2.5 days. For stars of various ages from 107.5 to1010.2 yr the maximum circularized periods are a smoothexponential function of age.
| The presence of Nd and Pr in HgMn stars
Optical region spectra for a number of upper main sequence chemicallypeculiar (CP) stars have been observed to study singly and doublyionized praseodymium and neodymium lines. In order to improve existingatomic data of these elements, laboratory measurements have been carriedout with the Lund VUV Fourier Transform Spectrometer (FTS). From thesemeasurements wavelengths and hyperfine structure (hfs) have been studiedfor selected Pr Ii, Pr Iii and Nd Iii lines of astrophysical interest.Radiative lifetimes for some excited states of Pr Ii have beendetermined with the aid of laser spectroscopy at the Lund Laser Center(LLC) and have been combined with branching fractions measured in thelaboratory to calculate gf values for some of the stronger optical linesof Pr Ii. With the aid of the derived gf values and laboratorymeasurements of the hfs, a praseodymium abundance was derived fromselected Pr Ii lines in the spectrum of the Am star 32 Aqr. Thisabundance was used to derive astrophysical gf values for selected Pr Iiilines in 32 Aqr, and these gf values were used to get a praseodymiumabundance for the HgMn star HR 7775. The praseodymium abundance in HR7775 was then utilized to derive astrophysical gf values for allobservable Pr Iii lines in this star. The neodymium abundance, derivedfrom unblended lines of Nd Ii in HR 7775, has been utilized to establishastrophysical gf values for observed Nd Iii lines in the optical regionof this star. Selected Pr Iii and Nd Iii lines have been identified andstudied in a number of HgMn stars and three hot Am stars. Thepraseodymium and neodymium abundance change rapidly from an approximate1-1.2 dex enhancement for the hot Am stars to 1.5-3 dex enhancement forthe cool HgMn stars, indicating a well-defined boundary between the hotAm and HgMn stars in the vicinity of 10 500 K. The enhancement ofpraseodymium and neodymium in Am and HgMn stars may be explained bydiffusive processes active in the stellar atmosphere, while the observeddiscontinuity might be explained by a thin hydrogen convection zonethought to be present for the Am stars, but absent in the HgMn stars.The absence of a convection zone would cause the diffused elements togather higher in the atmosphere of HgMn stars compared to Am stars, andexplain the observed increase in abundance.
| New results of magnetic field diagnosis in HgMn stars and normal late B-type stars
We suggested in a previous paper that three HgMn stars, HD 175640, HD178065, and HD 186122, may be suspected to possess a magnetic field thatcould be larger than 2 kG. We report here new observations of thesethree stars, three more HgMn stars, and four normal late B-type stars.The search was carried out by measuring the equivalent width of the FeII lambda 6147.7 Å line relative to the equivalent width of the FeII lambda 6149.2 Å line. The observed relative differences betweenthe equivalent widths of these Fe II lines are compared with thosederived from synthetic spectra computed by neglecting magnetic fieldeffects. To investigate the effect of oscillator strength uncertaintieson the results, we computed equivalent widths by using both Fe II loggf-values taken from Kurucz & Bell (\cite{KB95}) and Fe II loggf-values taken from Raassen & Uylings (2000). The comparison of thecomputed and observed equivalent widths based on the Kurucz & Bell(\cite{KB95}) atomic data leads us to conclude that all the stars of oursample, except HD 175640, are very likely to possess a magnetic field.On the other hand, the comparison of the computed and observedequivalent widths based on the Raassen & Uylings (2000) loggf-values suggests the possible presence of magnetic fields only inthree stars, the HgMn star HD 16717 and the two normal B-type stars HD179761 and HD 186568. The latter two are those in the sample with thelargest vsin i (15 km s-1 and 18 km s-1,respectively), so that the results for them are the most uncertain ones.
| Neon abundances in normal late-B and mercury-manganese stars
We make new non-local thermodynamic equilibrium calculations to deducethe abundances of neon from visible-region echelle spectra of selectedNei lines in seven normal stars and 20HgMn stars. We find that the beststrong blend-free Ne line that can be used at the lower end of theeffective temperature Teff range is λ6402, althoughseveral other potentially useful Nei lines are found in the red regionof the spectra of these stars. The mean neon abundance in the normalstars (logA=8.10) is in excellent agreement with the standard abundanceof neon (8.08). However, in HgMn stars neon is almost universallyunderabundant, ranging from marginal deficits of 0.1-0.3dex tounderabundances of an order of magnitude or more. In many cases, thelines are so weak that only upper limits can be established. The mostextreme example found is υ Her with an underabundance of at least1.5dex. These underabundances are qualitatively expected from radiativeacceleration calculations, which show that Ne has a very small radiativeacceleration in the photosphere, and that it is expected to undergogravitational settling if the mixing processes are sufficiently weak andthere is no strong stellar wind. According to theoretical predictions,the low Ne abundances place an important constraint on the intensity ofsuch stellar winds, which must be less than10-14Msolaryr-1 if they arenon-turbulent.
| Emission lines in the spectra of late-B type stars
We report detections of weak emission lines in the red spectral regionof sharp-lined chemically normal and peculiar (HgMn) late-B type starsfrom high spectral resolution and high signal-to-noise data. Mostemission lines originate from high-excitation states of the ions Cr IIand Mn II, with others likely to be attributed to Ti II and Fe II. Theemission is observed to extend over the entire line profile width forrotational velocities up to 18 km s-1, implying that itoriginates within the same rotational framework as the absorption linespectrum. Within the sample no obvious correlation is noted for thepresence of emission with regard to stellar effective temperature orluminosity. A dependence upon element abundance is evident from theabsence of Mn II emission for HgMn stars for which the manganeseenhancement is greater than 1.3 dex. This trend is mildly reinforced bythe chromium emission spectrum being most developed amongst stars richerin chromium. We postulate that the Cr II and Mn II emissions in the redspectral region arise from a selective excitation process involvinghydrogen Lyalpha photon energies.
| Elemental abundance analyses with Complejo Astronomico El Leoncito REOSC echelle spectrograms. IV. Extensions of nine previous analyses
Using new CASLEO echelle spectrograms, we extended our elementalabundances of the sharp-lined Mercury-Manganese stars mu Lep, 14 Hya,kappa Cnc, HR 4487, HR 4817, 28 Her, and HR 7245, the closely relatedstar 3 Cen A, and 7 Sex an A0 V star with Population I abundances, butwith Population II star space motions. The lambda lambda 4500-6200region contains a sufficient number of lines to derive high-qualityabundances of these stars. For most stars, the new spectra provideadditional lines for the analyses which improve their quality as well ashelp fill in the periodic table. Table~5 is only available in electronicform at the CDS via anonymous ftp to cdsarc.u-strasbg.fr(130.79.128.5)or via http://cdsweb.u-strabg.fr/Abstract.html}
| Mercury Elemental and Isotopic Abundances in Mercury-Manganese Stars
Hg II abundances have been determined for 42 mercury-manganese (HgMn)stars by fitting synthetic spectra to observed spectra of the 3984Å Hg II line. Twenty of the stars had lines sharp enough to allowtheir Hg isotopic abundance mixes to be estimated. The Hg abundance isreported for more HgMn stars here than in any other single work. Nocorrelation was found between Hg II abundance and T_eff or the meancentral wavelength of HgMn lambda3984 stars. The mean central wavelengthof lambda3984 , an indicator of the Hg isotopic mix, is looselycorrelated with T_eff: stars with primarily heavy Hg isotopes tend to becooler, although one star, 46 Aql, has almost pure ^204Hg and T_eff inabout the middle of the temperature range for HgMn stars. We find thatthere is no evidence that any of the HgMn stars have ^196Hg or ^198Hg.For the very sharp-lined stars, the ^204Hg abundance decreases withincreasing T_eff. No correlation is seen between the mean centralwavelength and the surface gravity. No correlation was found between theprojected rotational velocity and the Hg II abundance or the centralwavelength of lambda3984, although this result may be biased by theselection of stars with low reported vsini. Hg I lambda4358 was measuredat high spectral resolution for seven HgMn stars. The isotopic shiftsare too small, and the hyperfine components are too weak to allowunambiguous isotopic abundance ratios to be found. Hg I abundancescorrelate fairly well with Hg II abundances. Some of the Hg isotopicmixtures are difficult to explain using only diffusion. HR 7245 hasapproximately equal abundances of ^199Hg, ^200Hg, ^202Hg, and ^204Hg butvery little ^201Hg, and 11 Per has Hg that is mostly ^199Hg and ^204Hg.Calculations show that hyperfine splitting of ^201Hg changes theradiative forces it feels compared with other isotopes, which may alterdiffusion of that isotope enough to explain its absence in HR 7245, butwe have found no possible explanation for the Hg isotopic mix found in11 Per. These are the first very high resolution measurements of Hg IIlambda3984 for HR 7245 and 11 Per. Although diffusion may be acting inHgMn stars, either there are one or more other mechanisms acting to helpproduce the overabundances and isotopic mixtures seen or ourunderstanding of diffusion is lacking on some important point.
| Three Very Young HGMN Stars in the Orion OB1 Association
We report the detection of three mercury-manganese stars in the OrionOB1 association. HD 37886 and BD -0 deg984 are in the approximately 1.7million year old Orion OB1b. HD 37492 is in the approximately 4.6million year old Orion OB1c. Orion OB1b is now the youngest cluster withknown HgMn star members. This places an observational upper limit on thetimescale needed to produce the chemical peculiarities seen inmercury-manganese stars, which should help in the search for the causeor causes of the peculiar abundances in HgMn and other chemicallypeculiar upper main-sequence stars.
| Speckle Interferometry of New and Problem HIPPARCOS Binaries
The ESA Hipparcos satellite made measurements of over 12,000 doublestars and discovered 3406 new systems. In addition to these, 4706entries in the Hipparcos Catalogue correspond to double star solutionsthat did not provide the classical parameters of separation and positionangle (rho,theta) but were the so-called problem stars, flagged ``G,''``O,'' ``V,'' or ``X'' (field H59 of the main catalog). An additionalsubset of 6981 entries were treated as single objects but classified byHipparcos as ``suspected nonsingle'' (flag ``S'' in field H61), thusyielding a total of 11,687 ``problem stars.'' Of the many ground-basedtechniques for the study of double stars, probably the one with thegreatest potential for exploration of these new and problem Hipparcosbinaries is speckle interferometry. Results are presented from aninspection of 848 new and problem Hipparcos binaries, using botharchival and new speckle observations obtained with the USNO and CHARAspeckle cameras.
| Search for magnetic fields in HgMn stars by using relative strengths of multiplet 74 Fe II lines
The anomalous strength of the Fe II lambda 6147.7 line relative to Fe IIlambda 6149.2 in the stars with magnetic fields is used for detectingmagnetic fields in very slowly rotating HgMn stars. The diagnosis basedon this pair of magnetically sensitive Fe lines is a simple and fasttool, but its application to more rapidly rotating HgMn stars ishampered by blending with Hg II lambda 6149.5. For spectra ofsharp-lined HgMn stars (with v sin i<4 km s(-1) ) taken at highresolving power (R>= 100 000) both lines, Fe II lambda 6149.25 and HgII lambda 6149.48, become fully unblended. The observed relativedifferences between the equivalent widths of the two Fe II lines arecompared with those derived from synthetic spectra computed byneglecting magnetic field effects. This comparison has shown that threeHgMn stars, HD 175640, HD 178065 and HD 186122 are very likely topossess a magnetic field that could be larger than 2 kG. Based onobservations obtained at the European Southern Observatory, La Silla,Chile (ESO programme No.~61.D-0480)
| On the HIPPARCOS photometry of chemically peculiar B, A, and F stars
The Hipparcos photometry of the Chemically Peculiar main sequence B, A,and F stars is examined for variability. Some non-magnetic CP stars,Mercury-Manganese and metallic-line stars, which according to canonicalwisdom should not be variable, may be variable and are identified forfurther study. Some potentially important magnetic CP stars are noted.Tables 1, 2, and 3 are available only in electronic form at the CDS viaanonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or viahttp://cdsweb.u-strasbg.fr/Abstract.html
| Delta a and Stroemgren photometry of stars in the Renson-catalogue of AP and AM stars
We have observed 131 stars of \cite[Renson's (1991)]{re91} catalogue ofAp and Am stars both in the Stroemgren & Maitzen's (1976) Delta asystem as a contribution to the photometric studies of the lambda 5200broad band flux depression feature in chemically peculiar stars. Withfew exceptions the probability grouping of Renson for membership in theCP2 group of peculiar stars is nicely reflected by peculiar values ofDelta a. Comparison with already available Delta a values yieldsslightly larger values due to a minor shift in the filter g_1 samplingthe depression. As found by \cite[Maitzen & Vogt (1983)]{ma83} theGeneva system peculiarity parameters correlate well with Delta a. Thisstudy demonstrates the advantageous performance of a photoelectricphotometer with a rapidly rotating filter wheel moving in a stop and gomode. Tables 3 and 4 are also available in electronic form at the CDSvia anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or viahttp://cdsweb.u-strasbg.fr/Abstract.html
| BVRIJHK Photometry of Cepheid Variables
Contemporaneous BVRI and JHK photometry are presented for twenty-twoCepheid variables. Nineteen of these variables also have uvby photometryavailable, making them excellent candidates for application of theInfrared Flux Method of distance determination. We are in the process ofacquiring high precision radial velocities of sixteen of these variablesin anticipation of conducting that analysi. (SECTION: Stars)
| Atomic data for interpretation of HgMn spectra: Transition probabilities of MN III
Transition probabilities of the spectrum of Mn III are calculated usingthe orthogonal operator description for both the odd and the even energylevels. The full Tables \ref{mn3,gf} and \ref{mn3,A} are only availablein electronic form at the CDS via anonymous ftp to cdsarc.u-strasbg.fr(130.79.128.5) or via http://cdsweb.u-strasbg.fr/Abstract.html
| A catalogue of [Fe/H] determinations: 1996 edition
A fifth Edition of the Catalogue of [Fe/H] determinations is presentedherewith. It contains 5946 determinations for 3247 stars, including 751stars in 84 associations, clusters or galaxies. The literature iscomplete up to December 1995. The 700 bibliographical referencescorrespond to [Fe/H] determinations obtained from high resolutionspectroscopic observations and detailed analyses, most of them carriedout with the help of model-atmospheres. The Catalogue is made up ofthree formatted files: File 1: field stars, File 2: stars in galacticassociations and clusters, and stars in SMC, LMC, M33, File 3: numberedlist of bibliographical references The three files are only available inelectronic form at the Centre de Donnees Stellaires in Strasbourg, viaanonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5), or viahttp://cdsweb.u-strasbg.fr/Abstract.html
| The 3He isotope in the atmospheres of HgMn stars.
Not Available
| The ROSAT all-sky survey catalogue of optically bright OB-type stars.
For the detailed statistical analysis of the X-ray emission of hot starswe selected all stars of spectral type O and B listed in the Yale BrightStar Catalogue and searched for them in the ROSAT All-Sky Survey. Inthis paper we describe the selection and preparation of the data andpresent a compilation of the derived X-ray data for a complete sample ofbright OB stars.
| Elemental abundance analyses with Complejo Astronomico. EL Leoncito REOSC echelle spectrograms. I. κ Cancri, HR 7245, and ξ Octantis
Elemental abundances are derived for three sharp-lined stars κCnc, HR 7245, and ξ Oct using REOSC echelle spectrograms obtained atCASLEO. Comparisons are made with published equivalent widths. Thederived abundances for κ Cnc and ξ Oct are slightly larger thanthose obtained with other high dispersion spectrographs. HR 7245exhibits a pattern of abundance anomalies similar to otherMercury-Manganese stars. The spectra of the two HgMn stars in theλλ4640-5100 region exhibit an interesting and usefulvariety of lines which can be used to supplement analyses of thephotographic region.
| 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.
| Study of Two Hgmn-Stars with Suspected Anomalies of Abundances of Noble Gases
Not Available
| A new library of stellar optical spectra
Attention is given to a new digital optical stellar library consistingof spectra covering 3510-8930 R at 11-A resolution for 72 differentstellar types. These types extend over the spectral classes O-M andluminosity classes I-V. Most spectra are of solar metallicity stars butsome metal-rich and metal-poor spectra are included. This new library isquantitatively compared to two previously published libraries. It offersseveral advantages over them: it is photometrically well-calibratedindividually and consistently from star to star. Good temperature andluminosity coverage has been achieved. The incorporation of stars withwell-determined temperature, metallicity, and surface gravity parametersincreases the accuracy of the spectral type assigned to each compositelibrary star.
| A catalogue of Fe/H determinations - 1991 edition
A revised version of the catalog of Fe/H determinations published by G.Cayrel et al. (1985) is presented. The catalog contains 3252 Fe/Hdeterminations for 1676 stars. The literature is complete up to December1990. The catalog includes only Fe/H determinations obtained from highresolution spectroscopic observations based on detailed spectroscopicanalyses, most of them carried out with model atmospheres. The catalogcontains a good number of Fe/H determinations for stars from open andglobular clusters and for some supergiants in the Magellanic Clouds.
| Carbon, nitrogen, and oxygen abundances in the chemically peculiar stars of the upper main sequence
Low-noise, high-resolution Reticon spectra are used to obtain C, N, andO abundances for chemically peculiar stars with surface temperaturesbetween 7,000 and 15,000 K. The analysis includes C I, C II, N I, and OI lines for 13 Am and related stars, nine Hg-Mn stars, 15 magnetic Apstars, and five standard stars. The C and O abundances show a roughlymonotonic increase with surface temperature. The C and O results are ingeneral agreement with radiative diffusion theory. The N abundances,however, show that N is slightly deficient in cool nonmagnetic stars andvery deficient above 10,000 K in nonmagnetic stars. The results for Ndisagree with simple diffusion predictions, suggesting that a moredetailed model is needed for partially ionized N near the stellarsurface.
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Observation and Astrometry data
| Constellation: | Adler |
| Right ascension: | 19h07m09.10s |
| Declination: | +00°38'30.0" |
| Apparent magnitude: | 6.56 |
| Distance: | 230.415 parsecs |
| Proper motion RA: | -2.8 |
| Proper motion Dec: | -13.9 |
| B-T magnitude: | 6.601 |
| V-T magnitude: | 6.544 |
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