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The Progenitor Masses of Wolf-Rayet Stars and Luminous Blue Variables Determined from Clust

The Progenitor Masses of Wolf-Rayet Stars and Luminous Blue Variables Determined from Clust
The Progenitor Masses of Wolf-Rayet Stars and Luminous Blue Variables Determined from Clust

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The Progenitor Masses of Wolf-Rayet Stars and Luminous Blue Variables Determined from Cluster Turn-o?s.II.Results from 12Galactic Clusters and OB Associations Philip Massey 1,2Kitt Peak National Observatory,National Optical Astronomy Observatory 3P.O.Box 26732,Tucson,AZ 85726-6732massey@https://www.doczj.com/doc/a9644957.html, Kathleen DeGioia-Eastwood 4and Elizabeth Waterhouse 4,5Department of Physics and Astronomy,Northern Arizona University P.O.Box 6010,Flagsta?,AZ 86011-6010.kathy.eastwood@https://www.doczj.com/doc/a9644957.html, waterh@https://www.doczj.com/doc/a9644957.html, Received

ABSTRACT

In a previous paper on the Magellanic Clouds we demonstrated that coeval clusters provide a powerful tool for probing the progenitor masses of Wolf-Rayet stars(W-Rs)and Luminous Blue Variables(LBVs).Here we extend this work to the higher metallicity regions of the Milky Way,studying12Galactic clusters. We present new spectral types for the unevolved stars and use these,plus data from the literature,to construct H-R diagrams.We?nd that all but two of the clusters are highly coeval,with the highest mass stars having formed over a period of less than1Myr.The turn-o?masses show that at Milky Way metallicities some W-Rs(of early WN type)come from stars with masses as low as20–25M⊙. Other early-type WNs appears to have evolved from high masses,suggesting a large range of masses evolve through an early-WN stage.On the other hand, WN7stars are found only in clusters with very high turn-o?masses,>120M⊙. Similarly the LBVs are only found in clusters with the highest turn-o?masses, as we found in the Magellanic Clouds,providing very strong evidence that LBVs are a normal stage in the evolution of the most massive stars.Although clusters containing WN7s and LBVs can be as young as1Myr,we argue that these objects are evolved,and that the young age simply re?ects the very high masses that characterize the progenitors of such stars.In particular we show that the LBVηCar appears to be coeval with the rest of the Trumpler14/16complex. Although the WCs in the Magellanic Clouds were found in clusers with turn-o?masses as low as45M⊙,the three Galactic WCs in our sample are all found in clusters with high turn-o?masses(>70M⊙);whether this di?erence is signi?cant or due to small-number statistics remains to be seen.The BCs of Galactic W-Rs are hard to establish using the cluster turn-o?method,but are consistent with the“standard model”of Hillier.

Subject headings:open clusters and associations:individual—stars:early-type

—stars:evolution—stars:Wolf-Rayet

1.Introduction

1.1.Background

Massive,luminous stars begin their H-burning lives as hot,O-type stars.During their main-sequence evolution(2.5–8Myr for stars with initial masses of120–20M⊙)they may lose a signi?cant amount of their mass due to strong stellar winds.The observed mass-loss rates suggest that the highest-mass stars will lose as much as half their mass during the H-burning stage.Since these winds are driven by radiation pressure through highly-ionized metal lines,the mass-loss rates will increase with stellar luminosity,metallicity,and e?ective temperature.It was Conti(1976)who?rst suggested that mass-loss provided a simple explanation for how Wolf-Rayet(W-R)stars form.In the modern version of the“Conti scenario”(Maeder&Conti1994),this mass loss results in a stripping o?of the H-rich outer layers of the star,resulting in a WN-type W-R star,in which the H-burning products(He and N)are enriched at the surface,with strong,broad emission lines indicative of enhanced stellar winds forming an extended atmosphere.Most WNs are presumed to be He-burning objects,although there is evidence that a few H-rich late-type WNs are still near the end of the core-H burning phase(Conti et al.1995).Further mass-loss and evolution reveals the products of He-burning(C and O)at the surface,and the star is spectroscopically identi?ed as a WC-type W-R.

Possibly the highest mass stars also go through a Luminous Blue Variable(LBV)stage on their way to becoming W-Rs,with the large,episodic mass loss that characterizes LBVs aiding the process.Stars of slightly lower luminosity(mass)will not have an LBV phase,

but recent observations(Massey1998a)suggest that they do go through an intermediate red supergiant(RSG)phase,even at high metallicities,albeit for a short time.At some lower luminosity one expects that the mass-loss rates are su?cient to produce a WN-type W-R,but not a WC.And,at even lower luminosities,mass-loss rates are so low that the He-burning stage is spent entirely as a red supergiant(RSG)and not as a W-R star.

In this version of the“Conti scenario”we thus might expect the following“paths”to be followed,in order of decreasing luminosities:

O?→LBV?→WN?→WC(1)

O?→RSG?→WN?→WC(2)

O?→RSG?→WN(3)

OB?→RSG(4)

The masses corresponding to these paths are unknown(and indeed we are unsure even of the qualitative correctness of these paths),but“standard guesses”for characteristic values would be1:≥80M⊙,2:60M⊙,3:40M⊙,and4:20M⊙.We emphasize that these are purely speculative values,and that the actual ranges should depend upon metallicity. Indeed it is to address this issue that the present series of papers has come about.

Between the initial O-type stage(of luminosity class“V”)and the He-burning stage (LBVs,W-Rs,RSGs)the star will become a B-type supergiant;most,but not all,of these are expected to still be H-burning objects(Massey et al.1995b).The luminous

A-F supergiants are very short-lived intermediate stages during He-burning for stars of intermediate high-mass,depending upon the metallicity.The precursor to SN1987A is believed to have been a“second-generation”B-type supergiant,a He-burning object of somewhat lower mass than those being discussed here.

In addition to the question of whether or not the above paths are correct,and what masses to assign to each as a function of metallicity,we are also interested in the evolutionary signi?cance,if any,to the Wolf-Rayet spectral subtypes.WN-type W-R stars are classi?ed as“early”(WNE)or“late”(WNL)depending on whether NVλλ4602,19 or NIIIλλ4634,42dominates;e.g.,WNEs correspond to numerical subtypes WN2,WN3, WN4,while WNLs consist of subtypes WN6,WN7,WN8,and WN9,with the WN5stars split between the two groups.Similarly WC-type W-R stars are classi?ed as WCE or WCL depending upon whether CIIIλ5696dominates over CIVλ5808;e.g.,corresponding to spectral subtypes WC4through WC6and WC8-9,with some WC7s falling into each camp(Conti&Massey1989).Do these subtypes mean anything in an evolutionary sense? Various authors have claimed so(see,for example,Mo?at1982),but this conjecture does not seem borne out by either observational or theoretical studies.

Our understanding of massive star evolution is limited,in part,because of the

di?culty of constructing stellar models from?rst principles.The physics of massive stars is complicated by strong stellar winds,and the choice of the functional dependence of mass-loss rates on stellar parameters(luminosity,temperature,mass,and metallicity) greatly in?uences the theoretical tracks(e.g.,Meynet et al.1994),particularly in the later stages of evolution.In addition,the models are sensitive to the amount of mixing.However, there is little agreement on the treatment of the relevant processes of semi-convection and overshooting(Maeder&Conti1994),while the most recent work has emphasized the signi?cant role that rotation may play in this regard(Maeder1997,1999).Nevertheless, empirical studies of massive star evolution provide con?dence that the above picture

is correct,and are beginning to provide quantitative information on the mass ranges corresponding the various paths.These studies provide an observational basis against which the models can be evaluated and re?ned.(For a humorous rendering of this process,the reader is referred to Fig.5in Conti1982.)

1.2.An Observational Approach

1.2.1.Global Studies

The galaxies of the Local Group provide perfect laboratories for pursing these studies observationally,as the metallicity di?ers by almost an order of magnitude(SMC to M31) among the galaxies currently active in forming stars.During the past few years there have been a number of studies of mixed-age populations,the relative number of this and that. The implicit assumption of these studies are that the IMF slopes are identical and cover regions that provide a good sampling of stellar stages over time.The number ratios provide quantitative criterion for the models to attempt to match.These studies have found the following:

(1)The relative number of RSGs to W-Rs decreases with increasing metallicity(Massey 1998a;Massey&Johnson1998).Histograms of the number of RSGs vs.luminosity reveal that there are proportionately fewer high luminosity RSGs at higher metallicity,while the lack of a sharp luminosity cut-o?supports the interpretation that as Z increases,massive stars spend a greater fraction of their He-burning phase as W-Rs,and a smaller fraction as RSGs,rather than there being a di?erence in the actual mass ranges that go through a RSG phase.This is why we indicated a RSG phase at high luminosities(path2above). Possibly even LBVs will go—or have gone—through a RSG phase,but this is unknown. We also do not know if massive stars go through a RSG phase at the highest metallicity: the relation between the RSG/W-R ratio and metallicity appears to?atten below the high metallicity that characterize M31,but only a few regions have been surveyed in that large galaxy,and more data are being gathered to resolve this.

(2)The relative number of WCs to WNs increases with increasing metallicity,with the notable exception of the star-burst galaxy IC10(Fig.8in Massey&Johnson1998).This

trend is also in accord with the predictions of the Conti scenario,as increased mass-loss makes it possible for a star of a given luminosity to reach the WC stage sooner,spending more of its W-R stage as a WC than a WN.(The explanation for IC10’s peculiarly high WC/WN ratio remains a mystery at present.See discussion in Massey&Johnson1998.)

(3)Signi?cant di?erences in the spectral subtypes found in the Magellanic Clouds compared to the Milky Way were noted by Smith(1968):no WCLs are found in the LMC or SMC,and most of the ones known in the Milky Way are found inwards of the solar circle.Similar di?erences are seen for the WNs.Armandro?&Massey(1991)showed that the WC line widths(which are correlated with spectral subclass)change systematically with metallicity,extending an important?nding by Willis,Schild,&Smith(1992)to other galaxies of the Local Group.Massey(1996)proposed that the WC spectral subtypes are nothing more than an atmospheric e?ect due to metallicity.(See also Massey&Johnson 1998).Recently Crowther(2000)has demonstrated from W-R model atmospheres that the WN subtypes may similarly be a re?ection of metallicity rather than other stellar parameters,at least in terms of WN3through WN6.

1.2.2.Coeval Associations

A more direct way exists to attack the problem of understanding massive star evolution. By using coeval associations that contain evolved,massive stars,we can in fact directly measure the mass ranges that correspond to the above evolutionary paths as a function of metallicity.This is the subject of the current series of papers.

In Paper I of this series(Massey,Waterhouse,&DeGioia-Eastwood2000)we established that many Magellanic Cloud OB associations and young clusters are su?ciently coeval(?τ<1Myr)that we can measure a meaningful cluster turn-o?mass;e.g.,the

mass of the most massive star on the main-sequence.These turn-o?masses then place a lower-limit on the mass of the progenitors of the evolved stars in the cluster,to the extent that star-formation proceeded coevally.If the cluster is well populated,than the initial mass of the turn-o?star is a good approximation to the initial mass of the progenitor of the W-R star.In addition,the bolometric luminosity of the cluster turn-o?sets useful limits on the bolometric corrections for the evolved stars,allowing tests of Wolf-Rayet model atmospheres,such as Hillier’s“standard model”(Hillier1987,1990).

The results were quite revealing.In a study of19OB associations in the Magellanic Clouds,we found that at the low metallicities that characterize the SMC,only the highest-mass stars(>70M⊙)become Wolf-Rayet stars,although the sample is small.This is equivalent to saying that path(3)above occurs only for M>70M⊙for Z≤0.005.6 At the higher metallicity of the LMC(Z=0.008),WN W-R stars come from stars with masses as low as30M⊙.We also found that WC stars are found in the same clusters as WNEs;e.g.,the lowest turn-o?mass found for a cluster containing WC stars was45M⊙, suggesting that stars with masses from30–45M⊙might correspond to path(3),while stars with masses45-85M⊙correspond to path(2).

The rare“Ofpe/WN9”stars7,once thought to be a transition type between“Of”stars and Wolf-Rayet stars,are only found in clusters and associations with the lowest turn-o?masses,25-35M⊙.Recently the Ofpe/WN9stars were implicated in the LBV phase of massive stars,after one Ofpe/WN9star(R127)underwent an“LBV-like”outburst.But, the classical LBVs in our LMC sample,including the archetype itself S Doradus,are found in clusters with the very highest turn-o?masses,>85M⊙.(Similarly the SMC W-R star HD5980,which many consider to be a“true”LBV[Barb′a et al.1995]is found in a cluster with a very high turn-o?mass.)We conclude that the Ofpe/WN9stars are just the lowest-mass versions of Wolf-Rayet stars.True LBVs,on the other hand,are found only in the clusters with the highest mass turn-o?s,suggesting that they are indeed stars near their Eddington limit and are a normal stage of the most massive stars.

Our study also shed light on the origin of the di?erent W-R classes and subtypes,

at least at the modest metallicity that characterizes the LMC.The early-type WN stars (WNEs)in the LMC are found in clusters with a large range of turn-o?masses(from30M⊙to100M⊙or more),suggesting that these are a stage that most massive stars go through at LMC-like metallicities.

We turn now to the higher metallicity of our own Milky Way,and pose the question of where do LBVs and Wolf-Rayets of various types come from at a metallicity considerably higher than that of the Magellanic Clouds.

2.The Sample

Previous attempts to use Galactic OB associations and clusters to measure the progenitor masses of W-R stars have been made by Schild&Maeder(1984),Humphreys, Nichols&Massey(1985),and Vazquez&Feinstein(1990);Smith,Meynet,&Mermilliod (1994)also discuss the issue but primarily with an emphasis on using the data for bolometric corrections.These studies relied upon results from the literature and did not obtain new spectroscopy of the cluster stars.Our experience,even in nearby young clusters,is that many of the high mass stars have been overlooked.8

In this paper we draw upon the literature,but also obtain new spectroscopy for the regions where this is required.We note that few of these regions have modern photometry. This is largely irrelevant for our purposes,as discussed further in Section2.2.2below,but does a?ect any attempts to use the distances as probes of Galactic structure.

2.1.Selection

For our sample,we began with the lists of W-Rs believed to be likely members of clusters and associations given by Lundstrom&Stenholm(1984)and Schild&Maeder (1984).We eliminated the many regions that lacked UBV photometry(unfortunately this excludes many?ne southern regions),were too big(NGC2439,Vul OB2),or were too sparse(the“HD155603Group”).This left us with12associations for which we either obtained new spectroscopy,or adequate data existed in the recent literature.We list these regions in Table1.

Two regions not listed in the table require special comment.First,we have excluded the region NGC3603from our study.NGC3603is the Milky Way’s answer to R136,

in that this is a young(1-2Myr),rich region that is so highly populated that the IMF extends up to very high masses.In both cases HST was needed for spatially resolving a single“WN+abs”star into multiple objects,and for obtaining spectra of the individual components.NGC3603contains several stars with WN6-like features,but whose individual luminosities are much higher than that of normal W-Rs of their type,and whose spectra show unmistakable evidence of hydrogen,also not in accord with their type.(This can be inferred from Fig.2in Drissen et al.1995,although the signi?cance at the the time was not apparent.)Massey&Hunter(1998)found the same thing in R136,and realized that these WN stars were simply“super Of”stars—core-H burning objects whose very large luminosities(corresponding to masses well above the120M⊙limits of published evolutionary tracks)result in such strong stellar winds that their spectral appearance mimics that of Wolf-Rayet stars.(The same conclusion is reached by de Koter,Heap,

&Hubeny1997.)An excellent comparison between the NGC3603and R136objects is provided by Crowther&Dessart(1998).We ignore these objects here,primarily as we do not consider them true Wolf-Rayet stars.

We also call attention to the cluster NGC6231(the nucleus of the large Sco OB1 association),which contains two Wolf-Rayet stars,the WN7star HD151932,and the WC7+O5-8binary HD155720.Although the cluster has received recent photometric attention(Perry,Hill,&Christodoulou1991;Sung,Bessell,&Lee1998;Baume,Vazquez &Feinstein1999),there is no modern spectroscopic study of this highly interesting region. Such a study would bolster or refute claims of large age spreads and peculiar mass functions in this cluster,as well as potentially providing additional information on the progenitor masses of Wolf-Rayet stars.

2.2.New Data:Spectral Types and Improved Distances and Reddenings

2.2.1.Spectral Types:New Data and Classi?cation

Owing to the recent study of a number of northern hemisphere OB young clusters and OB associations(Massey et al.1995a and references therein),most of our new spectroscopy was obtained for stars in interesting southern OB associations.The majority of the new spectra were obtained on the CTIO1.5-m telescope with the Loral1K CCD(1200×800 pixels)spectrometer on1998Mar19(UT)with grating47in second order and a CuSO4 blocking?lter.The dispersion was0.56?A pixel?1,and the100μm slit(1.8arcsec)yielded a resolution of1.5?A(2.5pixels)with coverage from4035?A to4700?A.

Data were also obtained from Kitt Peak telescopes of the northern clusters(Berkeley87 and Ma50),as well as critical data for some stars in the southern associations,admittedly at very low elevations.Most of these were obtained on the Mayall4-m during1998Sept 11-14.The RC Spectrograph was used with the T2KB detector(2048×2048pixels),with grating KP-22used in second order and a CuSO4blocking?lter.The dispersion was0.72?A pixel?1,and the300μm(2.0arcsec)slit yielded a resolution of1.8?A(2.5pixels),with

coverage from3750?A to5000?A being in good focus.

A few data were also obtained on the Kitt Peak2.1-m telescope1998July19and21, and on2000Mar17,using the“GoldCam”spectrometer with its Loral3K x1K CCD. Grating47was used in second order with a dispersion of0.47?A pixel?1,and the250μm(3 arcsec)slit provided a resolution of1.9?A(4pixels).The wavelength coverage was3800?A to4800?A.

Thus in all cases the wavelength range covered the important classi?cation lines

Si IVλ4089to He IIλ4686,at resolutions of1.5–1.9?A.

Good?at-?elding was provided by exposures of an illuminated white spot.Wavelength calibration was by means of He-Ar(CTIO)or He-Ne-Ar(KPNO)lamps.The customary IRAF optimal-extraction routines were used.We usually achieved a S/N of80per spectral resolution element.We classi?ed the stars based upon the criterion given in Walborn& Fitzpatrick(1990).

We list in Table2the brightest stars in each of these associations,including our new spectral types plus any from the literature.We have measured accurate coordinates from the Space Telescope Science Institute’s Digitized Sky Survey images,and include these in Table2to facilitate exact identi?cation.We describe the most interesting spectra here.

Two Newly Discovered O3Stars.The“O3”class was introduced by Walborn(1971) as an extension of the MK classes to hotter e?ective temperatures.At modest resolution and signal-to-noise(S/N),the spectra show no He I lines,but rather strong He II.The class is clearly degenerate,as higher resolution and better S/N shows He Iλ4471with equivalent widths as large as120-250m?A in some stars(Kudritizki1980;Simon et al.1983),and less than75m?A in others(i.e.,Paper I).Since the O3class represents the hottest class,all members are of high mass,and stars of type O3III and O3I must be of extremely high

mass.Such stars are correspondingly rare,with only?ve possible examples in the Milky Way(e.g.,the four mentioned by Walborn1994plus one other possible example discovered by Massey&Johnson1993in Tr14/16).

Thus,our discovery here of two additional such stars,both in the poorly studied cluster Pis24(Sec.2.3.6)is of some interest.We illustrate the spectra of these two stars, Pis24-1and Pis24-17in Fig.1.In the case of HDE319718=Pis24-1,we do detect He I λ4471with an equivalent width of85m?A,comparable to that seen in the most extreme of Carina stars which originally de?ned the class.Pis24-1is clearly of type O3If*:the “f”as both N IIIλλ4634,42and He IIλ4686are seen in emission,and the“*”signifying N IVλ4058emission stronger than N III.Both features are luminosity indicators,thus resulting in the“I”luminosity class.Note also the strong N Vλλ4603,19absorption,which also appears to be stronger in O3stars of high luminosity,although one might expect there is also a strong temperature dependence for this line,which is not seen in O4stars,except at high luminosities.The star had been previously classi?ed as“O4(f)”by Lorret,Testor, &Niemela(1984),although in fact Vijapurkar&Drilling(1993)had suggested an“O3III”designation.

In the case of Pis24-17,we do not detect He I.We would argue that its luminosity class is intermediate between“III”and“I”:on the one hand,He IIλ4686is strongly in absorption while N III is in emission,suggesting an O3III(f*)classi?cation,given that the N IV emission is comparable in strength to that of N III.However,there is incredibly strong N V absorption,which would argue either for higher luminosity(or higher e?ective temperature?).Rather than attempt to introduce a II(f*)into the nomenclature,we classify the star as O3III(f*).We are indebted to Nolan Walborn for his insightful comments on this spectrum.This star was labeled”N35B”by Lortet et al.(1984),and classi?ed as

O4-5V.Doubtless the strong nebular He Iλ4471emission disguised the O3nature of this

and Pis24-1on their photographic spectra.

Other Early O-type Supergiants.We show in Fig.2a few of our other early

O-type supergiants.The spectra here can be compared to those illustrated in Walborn& Fitzpatrick(1990).These spectra,and the new types listed in Table2,emphasize the need for modern spectroscopic studies of early-type stars even within modest distances of the Sun.

2.2.2.Reddenings and Distances

In order to locate the stars in the H-R diagram and assign masses,we need to know their luminosities;for this,we need to know their distances and reddenings.

We have photometry(from the literature),and good spectral types(mostly new),for only the brightest dozen or so stars in each cluster(e.g.,Table2),with the exception of the clusters previously studied in order to determine their initial mass function.Main-sequence ?tting is of little use when dealing with stars this hot,as color information(even in the absence of reddening)provides little information about e?ective temperature.Instead, we derive distances and reddenings through the spectral types,adopting the absolute magnitude calibration discussed in Paper I,as well as the same intrinsic color calibration.

For each star with a spectral type in Table2,we computed the reddening and true distance modulus,and then eliminated any obvious outliers.Discrepant distances can be due either to misclassi?cation by a luminosity class(relatively easy for the early B stars) or non-membership;multiplicity must also play an occasional role.The results are given in Table1,along with the other data on the clusters.We have also included an estimate of the

size of the region.In general,the determination of the distance moduli is good to0.1mag9.

2.3.Discussion of Individual Clusters

2.3.1.Ruprecht44(C0757?284)

The Ru44cluster has been described by Mo?at&FitzGerald(1974),FitzGerald

&Mo?at(1976),Havlen(1976),and Turner(1981);see also McCarthy&Miller(1974). The cluster is a condensation in the Pup OB2association.The WN4.5star WR10 (HD65865=MR11)is listed by Mo?at&FitzGerald as a member,although it lies well outside the central part of the cluster.(The“core”as shown in Fig.1of Mo?at& FitzGerald has a radius of6.4arcmin;the W-R star lies14arcmin to the SE of its center.) Distance estimates have ranged from the large values of Mo?at&FitzGerald(1974)and FitzGerald&Mo?at(1976)who proposed distance moduli of14.1–14.2mag(6.6–6.8kpc), to the smaller value of13.2mag(4.3kpc)found by Havlen(1976).The most recent and complete study is that of Turner(1981),who?nds a distance modulus of13.3mag(4.7kpc) from main-sequence?tting,in accord with the Hβvalue of Havlen.

Many of the existing spectral types in the cluster are listed by Mo?at&FitzGerald (1974)and Turner(1981)as uncertain,and we obtained new spectral information for eight stars.We?nd that the stars described as O-type are generally no earlier than B-type;for instance the star LSS909described as“O6:e”by Mo?at&FitzGerald,and revised to“O8”by Turner,is actually a B1V according to our CCD spectroscopy,and is likely a foreground object.(It was included as one of the outlying possible members by Turner.)Similarly, the star LSS899(Ru44-182)was classi?ed by Mo?at&FitzGerald(1974)as“O8V”,but subsequently reclassi?ed as B0V by Reed&FitzGerald(1983).On the other hand,the star LSS891(Ru44-183)was called“O9.5”by FitzGerald&Mo?at(1976)is actually an O8III(f)according to our spectroscopy,similar to the O8V classi?cation by Reed& FitzGerald(1983).Our derived distance modulus of13.35mag is in excellent accord with that found by Turner(1981).

2.3.2.Collinder228(C1041?597)

Cr228is just south of theηCarinae clusters Tr14and Tr16,and Cr232;see Figure1 in Massey&Johnson(1993).An excellent spectroscopic study of this region was conducted by Walborn(1973a,1982).In constructing our list of members,we began with the UBV photometry of Feinstein,Marraco,&Forte(1976).(The photometry of HD93146comes from Turner&Mo?at1980.)Spectral types are from Walborn(1973a,1982),as well as Levato&Malaroda(1981),with a few additional types from Tapia et al.(1988)based upon unspeci?ed sources.To this we add our own16new spectral types,mostly of stars with previous spectroscopy;the agreement between di?erent sources is generally very good. We eliminate stars thought to be non-members based on spectra or color,as indicated by Tapia et al.We also ignore the plethora of stars with late-B or early-A dwarf spectral types in determining the distance modulus or constructing the HRD.The resulting true distance modulus is12.45mag(3.1kpc)and the average color excess E(B?V)=0.37. (Our apparent distance modulus,13.6mag,is identical with that found by Tapia et al.but the true distance modulus is somewhat greater since they derive a higher average reddening for Cr228based upon calculating E(B?V)from their measured E(V?K)values.)Our distance modulus would place the cluster at essentially the same distance as the rest of the ηCar complex;see Massey&Johnson1993).A few of the stars have luminosity classes or reddenings inconsistent with the adopted distance,but the corrections are minor and probably all of these stars with spectral types are members.The W-R member is WR24,of type WN7.

2.3.3.Trumpler14/16

The LBV starηCarinae is part of the Tr14/16complex,as is the W-R star

HD93162=WR25(WN7+abs).Massey&Johnson(1993)provide a modern CCD study

of this region,including spectroscopy of many of the brightest blue stars,concluding that Tr14and Tr16were at the identical distance and were coeval.A comprehensive study of the fainter members is given by DeGioia-Eastwood et al.(2001),who study several background?elds in order to recognize pre-mainsequence objects in the HRD.

2.3.4.Pismis20(C1511?588)

The only previous photometry of Pismis20is the photographic study by Mo?at&Vogt (1973).WR67=HD134877=Pis20-8(WN6)is nearly2arcmin from the central core of the cluster,which is heavily concentrated in a region roughly1arcminute in diameter.We derive a distance modulus of12.7mag(3.5kpc)for the cluster,and an average reddening of E(B-V)=1.1,with little scatter.The reddening of WR67given by Conti&Vacca(1990)is identical with this value,and we?nd M v=?5.1,consistent with that expected for a WN6 star(Table II of Conti&Vacca1990).We conclude WR67is a member.Van der Hucht et al.(1981)also list WR66as a possible member,but its location some46arcminutes south of the cluster makes this extremely unlikely.

2.3.5.C1715?387

The cluster was studied by Havlen&Mo?at(1977),who identi?ed15members and9 non-members from their photoelectric UBV photometry.The cluster appears to contain two Wolf-Rayet stars,WR89(=LSS4065=C1715?387-1),of type WN710and WR87(=LSS 4064=C1715?387-3),also of type WN7.Their spectroscopy identi?ed several early-type

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If we take only the two O dwarfs,we?nd a distance modulus of12.0mag;the distances of the supergiants are consistent with this,although they would nominally suggest a distance modulus of12.2mag.We adopt a distance modulus of12.0mag(2.5kpc), identical to value obtained by Havlen&Mo?at(1977)using the same data but with less complete spectroscopic data.

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聚合诸侯捍卫中原,匡正天下功业千秋。号令诸侯以匡周室,主要靠的不是 武力。 行为磊落不欺诈,美德流传于身后。孔子赞美齐桓公,也称赞管仲。 百姓深受恩惠,天子赐肉与桓公,命其无拜来接受。桓公称小白不敢,天子 威严就在咫尺前。 晋文公继承来称霸,亲身尊奉周天王。周天子赏赐丰厚,仪式隆重。 接受玉器和美酒,弓矢武士三百名。晋文公声望镇诸侯,从其风者受尊重。 威名八方全传遍,名声仅次于齐桓公。佯称周王巡狩,招其天子到河阳,因 此大众议论纷纷。 赏析 《短歌行》 (“周西伯昌”)主要是曹操向内外臣僚及天下表明心 迹,当他翦灭群凶之际,功高震主之时,正所谓“君子终日乾乾,夕惕若 厉”者,但东吴孙权却瞅准时机竟上表大说天命而称臣,意在促曹操代汉 而使其失去“挟天子以令诸侯”之号召, 故曹操机敏地认识到“ 是儿欲据吾著炉上郁!”故曹操运筹谋略而赋此《短歌行 ·周西伯 昌》。 西伯姬昌在纣朝三分天下有其二的大好形势下, 犹能奉事殷纣, 故孔子盛称 “周之德, 其可谓至德也已矣。 ”但纣王亲信崇侯虎仍不免在纣王前 还要谗毁文王,并拘系于羑里。曹操举此史实,意在表明自己正在克心效法先圣 西伯姬昌,并肯定他的所作所为,谨慎惕惧,向来无愧于献帝之所赏。 并大谈西伯姬昌、齐桓公、晋文公皆曾受命“专使征伐”。而当 今天下时势与当年的西伯、齐桓、晋文之际颇相类似,天子如命他“专使 征伐”以讨不臣,乃英明之举。但他亦效西伯之德,重齐桓之功,戒晋文 之诈。然故作谦恭之辞耳,又谁知岂无更讨封赏之意乎 ?不然建安十八年(公元 213 年)五月献帝下诏曰《册魏公九锡文》,其文曰“朕闻先王并建明德, 胙之以土,分之以民,崇其宠章,备其礼物,所以藩卫王室、左右厥世也。其在 周成,管、蔡不静,惩难念功,乃使邵康公赐齐太公履,东至于海,西至于河, 南至于穆陵,北至于无棣,五侯九伯,实得征之。 世祚太师,以表东海。爰及襄王,亦有楚人不供王职,又命晋文登为侯伯, 锡以二辂、虎贲、斧钺、禾巨 鬯、弓矢,大启南阳,世作盟主。故周室之不坏, 系二国是赖。”又“今以冀州之河东、河内、魏郡、赵国、中山、常 山,巨鹿、安平、甘陵、平原凡十郡,封君为魏公。锡君玄土,苴以白茅,爰契 尔龟。”又“加君九锡,其敬听朕命。” 观汉献帝下诏《册魏公九锡文》全篇,尽叙其功,以为其功高于伊、周,而 其奖却低于齐、晋,故赐爵赐土,又加九锡,奖励空前。但曹操被奖愈高,心内 愈忧。故曹操在曾早在五十六岁写的《让县自明本志令》中谓“或者人见 孤强盛, 又性不信天命之事, 恐私心相评, 言有不逊之志, 妄相忖度, 每用耿耿。

2008年浙师大《外国文学名著鉴赏》期末考试答案

(一)文学常识 一、古希腊罗马 1.(1)宙斯(罗马神话称为朱庇特),希腊神话中最高的天神,掌管雷电云雨,是人和神的主宰。 (2)阿波罗,希腊神话中宙斯的儿子,主管光明、青春、音乐、诗歌等,常以手持弓箭的少年形象出现。 (3)雅典那,希腊神话中的智慧女神,雅典城邦的保护神。 (4)潘多拉,希腊神话中的第一个女人,貌美性诈。私自打开了宙斯送她的一只盒子,里面装的疾病、疯狂、罪恶、嫉妒等祸患,一齐飞出,只有希望留在盒底,人间因此充满灾难。“潘多拉的盒子”成为“祸灾的来源”的同义语。 (5)普罗米修斯,希腊神话中造福人间的神。盗取天火带到人间,并传授给人类多种手艺,触怒宙斯,被锁在高加索山崖,受神鹰啄食,是一个反抗强暴、不惜为人类牺牲一切的英雄。 (6)斯芬克司,希腊神话中的狮身女怪。常叫过路行人猜谜,猜不出即将行人杀害;后因谜底被俄底浦斯道破,即自杀。后常喻“谜”一样的人物。与埃及狮身人面像同名。 2.荷马,古希腊盲诗人。主要作品有《伊利亚特》和《奥德赛》,被称为荷马史诗。《伊利亚特》叙述十年特洛伊战争。《奥德赛》写特洛伊战争结束后,希腊英雄奥德赛历险回乡的故事。马克思称赞它“显示出永久的魅力”。 3.埃斯库罗斯,古希腊悲剧之父,代表作《被缚的普罗米修斯》。6.阿里斯托芬,古希腊“喜剧之父”代表作《阿卡奈人》。 4.索福克勒斯,古希腊重要悲剧作家,代表作《俄狄浦斯王》。5.欧里庇得斯,古希腊重要悲剧作家,代表作《美狄亚》。 二、中世纪文学 但丁,意大利人,伟大诗人,文艺复兴的先驱。恩格斯称他是“中世纪的最后一位诗人,同时又是新时代的最初一位诗人”。主要作品有叙事长诗《神曲》,由地狱、炼狱、天堂三部分组成。《神曲》以幻想形式,写但丁迷路,被人导引神游三界。在地狱中见到贪官污吏等受着惩罚,在净界中见到贪色贪财等较轻罪人,在天堂里见到殉道者等高贵的灵魂。 三、文艺复兴时期 1.薄迦丘意大利人短篇小说家,著有《十日谈》拉伯雷,法国人,著《巨人传》塞万提斯,西班牙人,著《堂?吉诃德》。 2.莎士比亚,16-17世纪文艺复兴时期英国伟大的剧作家和诗人,主要作品有四大悲剧——《哈姆雷特》、《奥赛罗》《麦克白》、《李尔王》,另有悲剧《罗密欧与朱丽叶》等,喜剧有《威尼斯商人》《第十二夜》《皆大欢喜》等,历史剧有《理查二世》、《亨利四世》等。马克思称之为“人类最伟大的戏剧天才”。 四、17世纪古典主义 9.笛福,17-18世纪英国著名小说家,被誉为“英国和欧洲小说之父”,主要作品《鲁滨逊漂流记》,是英国第一部现实主义长篇小说。10.弥尔顿,17世纪英国诗人,代表作:长诗《失乐园》,《失乐园》,表现了资产阶级清教徒的革命理想和英雄气概。 25.拉伯雷,16世纪法国作家,代表作:长篇小说《巨人传》。 26.莫里哀,法国17世纪古典主义文学最重要的作家,法国古典主义喜剧的创建者,主要作品为《伪君子》《悭吝人》(主人公叫阿巴公)等喜剧。 五、18世纪启蒙运动 1)歌德,德国文学最高成就的代表者。主要作品有书信体小说《少年维特之烦恼》,诗剧《浮士德》。 11.斯威夫特,18世纪英国作家,代表作:《格列佛游记》,以荒诞的情节讽刺了英国现实。 12.亨利·菲尔丁,18世纪英国作家,代表作:《汤姆·琼斯》。 六、19世纪浪漫主义 (1拜伦, 19世纪初期英国伟大的浪漫主义诗人,代表作为诗体小说《唐璜》通过青年贵族唐璜的种种经历,抨击欧洲反动的封建势力。《恰尔德。哈洛尔游记》 (2雨果,伟大作家,欧洲19世纪浪漫主义文学最卓越的代表。主要作品有长篇小说《巴黎圣母院》、《悲惨世界》、《笑面人》、《九三年》等。《悲惨世界》写的是失业短工冉阿让因偷吃一片面包被抓进监狱,后改名换姓,当上企业主和市长,但终不能摆脱迫害的故事。《巴黎圣母院》 弃儿伽西莫多,在一个偶然的场合被副主教克洛德.孚罗洛收养为义子,长大后有让他当上了巴黎圣母院的敲钟人。他虽然十分丑陋而且有多种残疾,心灵却异常高尚纯洁。 长年流浪街头的波希米亚姑娘拉.爱斯梅拉达,能歌善舞,天真貌美而心地淳厚。青年贫诗人尔比埃尔.甘果瓦偶然同她相遇,并在一个更偶然的场合成了她名义上的丈夫。很有名望的副教主本来一向专心于"圣职",忽然有一天欣赏到波希米亚姑娘的歌舞,忧千方百计要把她据为己有,对她进行了种种威胁甚至陷害,同时还为此不惜玩弄卑鄙手段,去欺骗利用他的义子伽西莫多和学生甘果瓦。眼看无论如何也实现不了占有爱斯梅拉达的罪恶企图,最后竟亲手把那可爱的少女送上了绞刑架。 另一方面,伽西莫多私下也爱慕着波希米亚姑娘。她遭到陷害,被伽西莫多巧计救出,在圣母院一间密室里避难,敲钟人用十分纯朴和真诚的感情去安慰她,保护她。当她再次处于危急中时,敲钟人为了援助她,表现出非凡的英勇和机智。而当他无意中发现自己的"义父"和"恩人"远望着高挂在绞刑架上的波希米亚姑娘而发出恶魔般的狞笑时,伽西莫多立即对那个伪善者下了最后的判决,亲手把克洛德.孚罗洛从高耸入云的钟塔上推下,使他摔的粉身碎骨。 (3司汤达,批判现实主义作家。代表作《红与黑》,写的是不满封建制度的平民青年于连,千方百计向上爬,最终被送上断头台的故事。“红”是将军服色,指“入军界”的道路;“黑”是主教服色,指当神父、主教的道路。 14.雪莱,19世纪积极浪漫主义诗人,欧洲文学史上最早歌颂空想社会主义的诗人之一,主要作品为诗剧《解放了的普罗米修斯》,抒情诗《西风颂》等。 15.托马斯·哈代,19世纪英国作家,代表作:长篇小说《德伯家的苔丝》。 16.萨克雷,19世纪英国作家,代表作:《名利场》 17.盖斯凯尔夫人,19世纪英国作家,代表作:《玛丽·巴顿》。 18.夏洛蒂?勃朗特,19世纪英国女作家,代表作:长篇小说《简?爱》19艾米丽?勃朗特,19世纪英国女作家,夏洛蒂?勃朗特之妹,代表作:长篇小说《呼啸山庄》。 20.狄更斯,19世纪英国批判现实主义文学的重要代表,主要作品为长篇小说《大卫?科波菲尔》、《艰难时世》《双城记》《雾都孤儿》。21.柯南道尔,19世纪英国著名侦探小说家,代表作品侦探小说集《福尔摩斯探案》是世界上最著名的侦探小说。 七、19世纪现实主义 1、巴尔扎克,19世纪上半叶法国和欧洲批判现实主义文学的杰出代表。主要作品有《人间喜剧》,包括《高老头》、《欧也妮·葛朗台》、《贝姨》、《邦斯舅舅》等。《人间喜剧》是世界文学中规模最宏伟的创作之一,也是人类思维劳动最辉煌的成果之一。马克思称其“提供了一部法国社会特别是巴黎上流社会的卓越的现实主义历史”。

(完整版)the的用法

定冠词the的用法: 定冠词the与指示代词this ,that同源,有“那(这)个”的意思,但较弱,可以和一个名词连用,来表示某个或某些特定的人或东西. (1)特指双方都明白的人或物 Take the medicine.把药吃了. (2)上文提到过的人或事 He bought a house.他买了幢房子. I've been to the house.我去过那幢房子. (3)指世界上独一无二的事物 the sun ,the sky ,the moon, the earth (4)单数名词连用表示一类事物 the dollar 美元 the fox 狐狸 或与形容词或分词连用,表示一类人 the rich 富人 the living 生者 (5)用在序数词和形容词最高级,及形容词等前面 Where do you live?你住在哪? I live on the second floor.我住在二楼. That's the very thing I've been looking for.那正是我要找的东西. (6)与复数名词连用,指整个群体 They are the teachers of this school.(指全体教师) They are teachers of this school.(指部分教师) (7)表示所有,相当于物主代词,用在表示身体部位的名词前 She caught me by the arm.她抓住了我的手臂. (8)用在某些有普通名词构成的国家名称,机关团体,阶级等专有名词前 the People's Republic of China 中华人民共和国 the United States 美国 (9)用在表示乐器的名词前 She plays the piano.她会弹钢琴. (10)用在姓氏的复数名词之前,表示一家人 the Greens 格林一家人(或格林夫妇) (11)用在惯用语中 in the day, in the morning... the day before yesterday, the next morning... in the sky... in the dark... in the end... on the whole, by the way...

外国名著赏析论文

题目:浅析从简爱到女性的尊严和爱 学院工商学院 专业新闻学3 学号 姓名闫万里 学科外国文学名着赏析 [摘要] 十九世纪中期,英国伟大的女性存在主义先驱,着名作家夏洛蒂勃朗特创作出了她的代表作--《简爱》,当时轰动了整个文坛,它是一部具有浓厚浪漫主义色彩的现实主义小说,被认为是作者"诗意的生平"的写照。它在问世后的一百多年里,它始终保持着历史不败的艺术感染力。直到现在它的影响还继续存在。在作品的序幕、发展、高潮和结尾中,女主人公的叛逆、自由、平等、自尊、纯洁的个性都是各个重点章节的主旨,而这些主旨则在女主人公的爱情观中被展露的淋漓尽致,它们如同乌云上方的星汉,灼灼闪耀着光芒,照亮着后来的女性者们追求爱情的道路。? [关键词] 自尊个性独特新女性主义自由独立平等 《简爱》是一部带有自转色彩的长篇小说,它阐释了这样一个主题:人的价值=尊严+爱。从小就成长在一个充满暴力的环境中的简爱,经历了同龄人没有的遭遇。她要面对的是舅妈的毫无人性的虐待,表兄的凶暴专横和表姐的傲慢冷漠,尽管她尽力想“竭力赢得别人的好感”,但是事实告诉她这都是白费力气的,因此她发出了“不公平啊!--不公平!”的近乎绝望的呼喊。不公平的生长环境,使得简爱从小就向往平等、自由和爱,这些愿望在她后来的成长过程中表现无疑,

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