Wolf–Rayet stars (often referred to as WR stars) are a heterogeneous set of stars with unusual spectra showing prominent broad emission lines of highly ionised helium and nitrogen or carbon. The spectra indicate very high surface temperatures of 30,000 K to around 200,000 K, surface enhancement of heavy elements, and strong stellar winds.
Classic (or Population I) Wolf–Rayet stars are evolved, massive stars, O-type stars over 20 solar masses when they were on the main sequence, that have now completely lost their outer hydrogen and are fusing helium or heavier elements in the core. A subset of WR stars are the central stars of planetary nebulae (CSPNe), post Asymptotic Giant Branch stars that were similar to the Sun while on the main sequence, but have now ceased fusion and shed their atmospheres to show a bare carbon-oxygen core. Another group (type WNh) show hydrogen lines in their spectra and are young extremely massive stars still fusing hydrogen at the core, with nitrogen mixed to the surface and strong radiation-driven mass loss. They are all highly luminous due to their high temperatures, thousands of times the bolometric luminosity of the Sun (L☉) for the CSPNe, hundreds of thousands L☉ for the Population I WR stars, to over a million L☉ for the WNh stars, although not exceptionally bright visually since most of their radiation output is in the ultraviolet.
In 1867, using the 40 cm Foucault telescope at the Paris Observatory, astronomers Charles Wolf and Georges Rayet discovered three stars in the constellation Cygnus (HD 191765, HD 192103 and HD 192641, now designated as WR 134, WR135, and WR137 respectively) that displayed broad emission bands on an otherwise continuous spectrum. Most stars only display absorption lines or bands in their spectra, as a result of overlying elements absorbing light energy at specific frequencies, so these were clearly unusual objects.
The nature of the emission bands in the spectra of a Wolf–Rayet star remained a mystery for several decades. Edward C. Pickering theorized that the lines were caused by an unusual state of hydrogen, and it was found that this "Pickering series" of lines followed a pattern similar to the Balmer series, when half-integral quantum numbers were substituted. It was later shown that the lines resulted from the presence of helium; a gas that was discovered in 1868. Pickering noted similarities between Wolf-Rayet spectra and nebular spectra, and this similarity led to the conclusion that some or all Wolf Rayet stars were the central stars of planetary nebulae.
By 1929, the width of the emission bands was being attributed to Doppler broadening, and hence that the gas surrounding these stars must be moving with velocities of 300–2400 km/s along the line of sight. The conclusion was that a Wolf–Rayet star is continually ejecting gas into space, producing an expanding envelope of nebulous gas. The force ejecting the gas at the high velocities observed is radiation pressure. It was well known that many stars with Wolf Rayet type spectra were the central stars of planetary nebulae, but also that many were not associated with an obvious planetary nebula or any visible nebulousity at all.
In addition to helium, emission lines of carbon, oxygen and nitrogen were identified in the spectra of Wolf–Rayet stars. In 1938, the International Astronomical Union classified the spectra of Wolf–Rayet stars into types WN and WC, depending on whether the spectrum was dominated by lines of nitrogen or carbon-oxygen respectively.
In 1969, several CSPNe with strong OVI emissions lines were grouped under a new "OVI sequence", or just OVI type. These were subsequently referred to as [WO] stars. Similar stars not associated with planetary nebulae were described shortly after and the WO classification was eventually also adopted for population I WR stars.
The understanding that certain late, and sometimes not-so-late, WN stars with hydrogen lines in their spectra are at a different stage of evolution from hydrogen-free WR stars has led to the introduction of the term WNh to distinguish these stars generally from other WN stars. They were previously referred to as WNL stars, although there are late-type WN stars without hydrogen as well as WR stars with hydrogen as early as WN5.
Wolf–Rayet stars were named on the basis of the strong broad emission lines in their spectra, identified with helium, nitrogen, carbon, silicon, and oxygen, but with hydrogen lines usually weak or absent. The first system of classification split these into stars with dominant lines of ionised nitrogen (NIII, NIV, and NV) and those with dominant lines of ionised carbon (CIII and CIV) and sometimes oxygen (OIII - OVI), referred to as WN and WC respectively. The two classes WN and WC were further split into temperature sequences WN5-WN8 and WC6-WC8 based on the relative strengths of the 541.1nm HeII and 587.5 nm HeI lines. Wolf-Rayet emission lines frequently have a broadened absorption wing (P Cygni profile) suggesting circumstellar material. A WO sequence has also been separated from the WC sequence for even hotter stars where emission of ionised oxygen dominates that of ionised carbon, although the actual proportions of those elements in the stars are likely to be comparable. WC and WO spectra are formally distinguished based on the presence or absence of CIII emission. WC spectra also generally lack the OVI lines that are strong in WO spectra.
The WN spectral sequence was expanded to include WN2 - WN9, and the definitions refined based on the relative strengths of the NIII lines at 463.4-464.1 nm and 531.4 nm, the NIV lines at 347.9-348.4 nm and 405.8 nm, and the NV lines at 460.3 nm, 461.9 nm, and 493.3-494.4 nm. These lines are well separated from areas of strong and variable He emission and the line strengths are well correlated with temperature. Stars with spectra intermediate between WN and Ofpe have been classified as WN10 and WN11 although this nomenclature is not universally accepted.
The type WN1 was proposed for stars with neither NIV nor NV lines, to accommodate Brey 1 and Brey 66 which appeared to be intermediate between WN2 and WN2.5. The relative line strengths and widths for each WN sub-class were later quantified, and the ratio between the 541.1 nm HeII and 587.5m, HeI lines was introduced as the primary indicator of the ionisation level and hence of the spectral sub-class. The need for WN1 disappeared and both Brey 1 and Brey 66 are now classified as WN3b. The somewhat obscure WN2.5 and WN4.5 classes were dropped.
|Spectral Type||Original criteria||Updated criteria||Other features|
|WN2||NV weak or absent||NV and NIV absent||Strong HeII, no HeI|
|WN2.5||NV present, NIV absent||Obsolete class|
|WN3||NIV ≪ NV, NIII weak or absent||HeII/HeI > 10, HeII/CIV > 5||Peculiar profiles, unpredictable NV strength|
|WN4||NIV ≈ NV, NIII weak or absent||4 < HeII/HeI < 10, NV/NIII > 2||CIV present|
|WN4.5||NIV > NV, NIII weak or absent||Obsolete class|
|WN5||NIII ≈ NIV ≈ NV||1.25 < HeII/HeI < 8, 0.5 < NV/NIII < 2||NIV or CIV > HeI|
|WN6||NIII ≈ NIV, NV weak||1.25 < HeII/HeI < 8, 2 < NIII/NV < 5||CIV ≈ HeI|
|WN7||NIII > NIV||0.65 < HeII/HeI < 1.25||Weak P-Cyg profile HeI, HeII > NIII, CIV > HeI|
|WN8||NIII ≫ NIV||HeII/HeI < 0.65||Strong P-Cyg profile HeI, HeII ≈ NIII, CIV weak|
|WN9||NIII > NII, NIV absent||NIII > NII, NIV absent||P-Cyg profile HeI|
|WN10||NIII ≈ NII||NIII ≈ NII||H Balmer, P-Cyg profile HeI|
|WN11||NIII weak or absent, NII present||NIII ≈ HeII, NIII weak or absent,||H Balmer, P-Cyg profile HeI, FeIII present|
The WC spectral sequence was expanded to include WC4 - WC11, although some older papers have also used WC1 - WC3. The primary emission lines used to distinguish the WC sub-types are CII 426.7 nm, CIII at 569.6 nm, CIII/IV465.0 nm, CIV at 580.1-581.2 nm, and the OV (and OIII) blend at 557.2-559.8 nm. The sequence was extended to include WC10 and WC11, and the subclass criteria were quantified based primarily on the relative strengths of carbon lines to rely on ionisation factors even if there were abundance variations between carbon and oxygen.
|Spectral type||Original criteria||Quantitative criteria||Other features|
|WC4||CIV strong, CII weak, OV moderate||CIV/CIII > 32||OV/CIII > 2.5||OVI weak or absent|
|WC5||CIII ≪ CIV, CIII < OV||12.5 < CIV/CIII < 32||0.4 < CIII/OV < 3||OVI weak or absent|
|WC6||CIII ≪ CIV, CIII > OV||4 < CIV/CIII < 12.5||1 < CIII/OV < 5||OVI weak or absent|
|WC7||CIII < CIV, CIII ≫ OV||1.25 < CIV/CIII < 4||CIII/OV > 1.25||OVI weak or absent|
|WC8||CIII > CIV, CII absent, OV weak or absent||0.5 < CIV/CIII < 1.25||CIV/CII > 10||HeII/HeI > 1.25|
|WC9||CIII > CIV, CII present, OV weak or absent||0.2 < CIV/CIII < 0.5||0.6 < CIV/CII < 10||0.15 < HeII/HeI < 1.25|
|WC10||0.06 < CIV/CIII < 0.15||0.03 < CIV/CII < 0.6||HeII/HeI < 0.15|
|WC11||CIV/CIII < 0.06||CIV/CII < 0.03||HeII absent|
For WO stars the main lines used are CIV at 580.1 nm, OIV at 340.0 nm, OV (and OIII) blend at 557.2-559.8 nm, OVI at 381.1-383.4 nm, OVII at 567.0 nm, and OVIII at 606.8 nm. The sequence was expanded to include WO5 and quantified based the relative strengths of the OVI/CIV and OVI/OV lines. A later scheme, designed for consistency across classical WR stars and CSPNe, returned to the WO1 to WO4 sequence and adjusted the divisions.
|Spectral type||Original criteria||Quantitative criteria||Other features|
|WO1||OVII ≥ OV, OVIII present||OVI/OV > 12.5||OVI/CIV > 1.5||OVII ≥ OV|
|WO2||OVII < OV, CIV < OVI||4 < OVI/OV < 12.5||OVI/CIV > 1.5||OVII ≤ OV|
|WO3||OVII weak or absent, CIV ≈ OVI||1.8 < OVI/OV < 4||0.1 < OVI/CIV < 1.5||OVII ≪ OV|
|WO4||CIV ≫ OVI||0.5 < OVI/OV < 1.8||0.03 < OVI/CIV < 0.1||OVII ≪ OV|
Detailed modern studies of Wolf Rayet stars can identify additional spectral features, indicated by suffixes to the main spectral classification:
- h for hydrogen emission;
- ha for hydrogen emission and absorption;
- w for weak lines;
- s for strong lines;
- b for broad strong lines;
- d for dust (occasionally vd, pd, or ed for variable, periodic, or episodic dust).
The classification of Wolf Rayet spectra is complicated by the frequent association of the stars with dense nebulosity, dust clouds, or binary companions. A suffix of "+OB" is used to indicate the presence of absorption lines in the spectrum likely to be associated with a more normal companion star, or "+abs" for absorption lines with an unknown origin.
The hotter WR spectral sub-classes are described as early and the cooler ones as late, consistent with other spectral types. WNE and WCE refer to early type spectra while WNL and WCL refer to late type spectra, with the dividing line approximately at sub-class six or seven. There is no such thing as a late WO star. There is a strong tendency for WNE stars to be hydrogen-poor while the spectra of WNL stars frequently include hydrogen lines.
Spectral types for the central stars of planetary nebulae are often qualified by surrounding them with square brackets (e.g. [WC2]). They are almost all of the WC sequence, with a very small number of [WO] and [WN] or [WC/WN] types. Temperatures tend to the extremes when compared to population I WR stars, so [WC2] and [WC3] are common and the sequence has been extended to [WC12]. The [WC11] and [WC12] types have distinctive spectra with narrow emission lines and no HeII and CIV lines.
Certain supernovae observed prior to their peak brightness show WR spectra. This is not surprising given the nature of the supernova at this point: a rapidly expanding helium-rich ejecta similar to an extreme Wolf Rayet wind. The WR spectral features only last a matter of hours, the high ionisation features fading by maximum to leave only weak neatral hydrogen and helium emission, before being replaced with a traditional supernova spectrum. It has been proposed to label these spectral types with an "X", for example XWN5(h). Similarly, classical novae develop spectra consisting of broad emission bands similar to a Wolf Rayet star. This is caused by the same physical mechanism: rapid expansion of dense gases around an extremely hot central source.
The first three Wolf Rayet stars to be identified, coincidentally all with hot O companions, had already been numbered in the HD catalogue. These stars and others were referred to as Wolf–Rayet stars from their initial discovery but specific naming conventions for them would not be created until 1962 in the "fourth" catalogue of galactic Wolf Rayet stars. The first three catalogues were not specifically lists of Wolf Rayet stars and they used only existing nomenclature. The fourth catalogue numbered the Wolf Rayet stars sequentially in order of right ascension. The fifth catalogue used the same numbers prefixed with MR after the author of the fourth catalogue, plus an additional sequence of numbers prefixed with LS for new discoveries. Neither of these numbering schemes is in common use.
The sixth Catalogue of Galactic Wolf Rayet stars was the first to actually bear that name, as well as to describe the previous five catalogues by that name. It also introduced the WR numbers widely used ever since for galactic WR stars. These are again a numerical sequence from WR 1 to WR 158 in order of right ascension. The seventh catalogue and its annex use the same numbering scheme and insert new stars into the sequence using lower case letter suffixes, for example WR 102ka for one of the numerous WR stars discovered in the galactic centre. Modern high volume identification surveys use their own numbering schemes for the large numbers of new discoveries. An IAU working group has accepted recommendations to expand the numbering system from the Catalogue of Galactic Wolf Rayet stars so that additional discoveries are given the closest existing WR number plus a numeric suffix in order of discovery. This applies to all discoveries since the 2006 annex, although some of these have already been named under the previous nomenclature; thus WR 42e is now numbered WR 42-1.
Wolf Rayet stars in external galaxies are numbered using different schemes. In the Large Magellanic Cloud, the most widespread and complete nomenclature for WR stars is from the fourth Catalogue of Population I Wolf Rayet stars in the Large Magellanic Cloud, prefixed by BAT-99, for example BAT-99 105. Many of these stars are also referred to by their third catalogue number, for example Brey 77. As of 2015, 152 WR stars are catalogued in the LMC, mostly WN but including three of the extremely rare WO class. Many of these stars are often referred to by their RMC (Radcliffe observatory Magellanic Cloud) numbers, frequently abbreviated to just R, for example R136a1.
In the Small Magellanic Cloud SMC WR numbers are used, usually referred to as AB numbers, for example AB7. There are only twelve known WR stars in the SMC, a very low number thought to be due to the low metallicity of that galaxy
A significant proportion of WR stars are surrounded by nebulosity associated directly with the star, not just the normal background nebulosity associated with any massive star forming region, and not a planetary nebula formed by a post-AGB star. The nebulosity presents a variety of forms and classification has been difficult. Many were originally catalogued as planetary nebulae and only careful study can distinguish a planetary nebula around a low mass post-AGB star from a similar nebula around a more massive core helium burning star.
Wolf–Rayet stars are a normal stage in the evolution of very massive stars, in which strong, broad emission lines of helium and nitrogen ("WN" sequence), carbon ("WC" sequence), and oxygen ("WO" sequence) are visible. Due to their strong emission lines they can be identified in nearby galaxies. About 500 Wolf–Rayets are catalogued in our own Milky Way Galaxy. This number has changed dramatically during the last few years as the result of photometric and spectroscopic surveys in the near-infrared dedicated to discovering this kind of object in the Galactic plane. It is expected that there are fewer than 1,000 WR stars in the rest of the Local Group galaxies, with around 150 known in the Magellanic Clouds, 206 in M33, and 154 in M31. Outside the local group, whole galaxy surveys have found thousands more WR stars and candidates. For example, over a thousand WR stars have been detected in M101, from magnitude 21 to 25. WR stars are expected to be particularly common in starburst galaxies and especially Wolf-Rayet galaxies.
The characteristic emission lines are formed in the extended and dense high-velocity wind region enveloping the very hot stellar photosphere, which produces a flood of UV radiation that causes fluorescence in the line-forming wind region. This ejection process uncovers in succession, first the nitrogen-rich products of CNO cycle burning of hydrogen (WN stars), and later the carbon-rich layer due to He burning (WC and WO stars).
It can be seen that the WNh stars are completely different objects from the WN stars without hydrogen. Despite the similar spectra, they are much more massive, much larger, and some of the most luminous stars known. They have been detected as early as WN5h in the Magellanic clouds. The nitrogen seen in the spectrum of WNh stars is still the product of CNO cycle fusion in the core, but it appears at the surface of the most massive stars due to rotational and convectional mixing while still in the core hydrogen burning phase, rather than after the outer envelope is lost during core helium fusion.
Some Wolf–Rayet stars of the carbon sequence ("WC"), especially those belonging to the latest types, are noticeable due to their production of dust. Usually this takes places on those belonging to binary systems as a product of the collision of the stellar winds forming the pair, as is the case of the famous binary WR 104; however this process occurs on single ones too.
A few (roughly 10%) of the central stars of planetary nebulae are, despite their much lower (typically ~0.6 solar) masses, also observationally of the WR-type; i.e., they show emission line spectra with broad lines from helium, carbon and oxygen. Denoted [WR], they are much older objects descended from evolved low-mass stars and are closely related to white dwarfs, rather than to the very young, very massive population I stars that comprise the bulk of the WR class. These are now generally excluded from the class denoted as Wolf–Rayet stars, or referred to as Wolf-Rayet type stars.
The numbers and properties of Wolf Rayet stars vary with the chemical composition of their progenitor stars. A primary driver of this difference is the rate of mass loss at different levels of metallicity. Higher metallicity leads to high mass loss, which affects the evolution of massive stars and also the properties of Wolf Rayet stars. Higher levels of mass loss cause stars to lose their outer layers before an iron core develops and collapses, so that the more massive red supergiants evolve back to hotter temperatures before exploding as a supernova, and the most massive stars never become red supergiants. In the Wolf Rayet stage, higher mass loss leads to stronger depletion of the layers outside the convective core, lower hydrogen surface abundances and more rapid stripping of helium to produce a WC spectrum.
These trends can be observed in the various galaxies of the local group, where metallicity varies from near-solar levels in the milky way, somewhat lower in M31, lower still in the Large Magellanic Cloud, and much lower in the Small Magellanic Cloud. Strong metallicity variations are seen across individual galaxies, with M33 and the milky way showing higher metallicities closer to the centre, and M31 showing higher metallicity in the disk than in the halo. Thus the SMC is seen to have few WR stars compared to its stellar formation rate and no WC stars at all (one star has a WO spectral type), the milky way has roughly equal numbers of WN and WC stars and a large total number of WR stars, and the other main galaxies have somewhat fewer WR stars and more WN than WC types. LMC, and especially SMC, Wolf Rayets have weaker emission and a tendency to higher atmospheric hydrogen fractions. SMC WR stars almost universally show some hydrogen and even absorption lines even at the earliest spectral types, due to weaker winds not entirely masking the photosphere.
The maximum mass of a main sequence star that can evolve through a red supergiant phase is calculated to be around 40 M☉ in the milky way and 65 M☉ or more in the SMC.
Mass loss is influenced by a star's rotation rate, especially strongly at low metallicity. Fast rotation contributes to mixing of core fusion products through the rest of the star, enhancing surface abundances of heavy elements, and driving mass loss. Rotation causes stars to remain on the main sequence longer than non-rotating stars, evolve more quickly away from the red supergiant phase, or even evolve directly from the main sequence to hotter temperatures for very high masses, high metallicity or very rapid rotation.
Stellar mass loss produces a loss of angular momentum and this quickly brakes the rotation of massive stars. Very massive stars at near-solar metallicity should be braked almost to a standstill while still on the main sequence, while at SMC metallicity they can continue to rotate rapidly even at the highest observed masses. Rapid rotation of massive stars may account for the unexpected properties and numbers of SMC WR stars, for example their relatively high temperatures and luminosities.
Massive stars in binary systems can develop into Wolf Rayet stars due to stripping by a companion rather than inherent mass loss due to a stellar wind. This process is relatively insensitive to the metallicity or rotation of the individual stars and is expected to produce a consistent set of WR stars across all the local group galaxies. As a result, the fraction of WR stars produced through the binary channel, and therefore the number of WR stars observed to be in binaries, should be higher in low metallicity environments. Calculations suggest that the binary fraction of WR stars observed in the SMC should be as high as 98%, although less than half are actually observed to have a massive companion. The binary fraction in the milky way is around, in line with theoretical calculations.
Theories about how WR stars form, develop, and die have been slow to form compared to the explanation of less extreme stellar evolution. They are rare, distant, and often obscured, and even into the 21st century many aspects of their lives are unclear.
Several astronomers, among them Rublev (1965) and Conti (1976) originally proposed that the WR stars as a class are descended from massive O-stars in which the strong stellar winds characteristic of extremely luminous stars have ejected the unprocessed outer H-rich layers. This has proved to be essentially correct, but with much complexity between a main sequence O star and the final WR star.
Early modelling of the evolution of massive stars showed that they evolve away from the main sequence, not towards hotter temperature and a WR state, but by expanding and cooling to become blue and then red supergiants. These supergiants are only modestly more luminous than the main sequence stars they originate from, but are progressively more unstable as their cores become hotter and their atmospheres more extended. Simple models of nuclear fusion showed that these red supergiants burned heavier elements in their cores until exploding as a supernova, but not becoming WR stars.
Further models showed that there was an upper limit to the stability of luminous stars. Sufficiently massive stars do not become red supergiants, instead shedding their atmospheres so quickly that they remain as blue supergiants, eventually shedding their atmospheres completely and entering the "Wolf Rayet funnel", an area of the Hertzsprung-Russell diagram where WR stars become progressively smaller and hotter as they shed more and more of their outer layers. The suggestion was that earlier and hotter stars were the later stages of evolution from the later and cooler WR stars, but the results of this evolutionary sequence didn't match observations very well.
Most WR stars, the classical population I type, are now understood as being a natural stage in the evolution of the most massive stars (not counting the less common planetary nebula central stars), either after a period as a red supergiant, after a period as a blue supergiant, or directly from the most massive main sequence stars. Only the lower mass red supergiants are expected to explode as a supernova at that stage, while more massive red supergiants progress back to hotter temperatures as they expel their atmospheres. Some explode while at the yellow hypergiant or LBV stage, but many become Wolf Rayet stars. They have lost or burnt almost all of their hydrogen and are now fusing helium in their cores, or heavier elements for a very brief period at the end of their lives.
Massive main sequence stars create a very hot core which fuses hydrogen very rapidly via the CNO process and results in strong convection throughout the whole star. This causes mixing of helium to the surface, a process that is enhanced by rotation, possibly by differential rotation where the core is spun up to a faster rotation than the surface. Such stars also show nitrogen enhancement at the surface at a very young age, caused by changes in the proportions of carbon and nitrogen due to the CNO cycle. The enhancement of heavy elements in the atmosphere, as well as increases in luminosity, create strong stellar winds which are the source of the emission line spectra. These stars develop an Of spectrum, Of* if they are sufficiently hot, which develops into a WNh spectrum as the stellar winds increase further. This explains the high mass and luminosity of the WNh stars, which are still burning hydrogen at the core and have lost little of their initial mass. These will eventually expand into blue supergiants (LBVs?) as hydrogen at the core becomes depleted, or if mixing is efficient enough (e.g. through rapid rotation) they may progress directly to WN stars without hydrogen.
Observations of supernovae reveal that around a quarter of core collapse supernovae are of Type Ib, originating from a progenitor with almost no hydrogen, and Type Ic, originating from a progenitor with almost no hydrogen and very little helium. This corresponds rather well to WC and WO stars and as this was investigated it appeared that WR stars were likely to end their lives violently rather than fade away to a neutron star. Thus every star with an initial mass more than about 9 times the sun would inevitably result in a supernova explosion, many of them from the WR stage.
A simple progression of WR stars from low to hot temperatures, resulting finally in WO stars, is not supported by observation. WO stars are extremely rare and all the known examples are more luminous and more massive than the relatively common WC stars. Alternative theories suggest either that the WO stars are only formed from the most massive main sequence stars, and/or that they form an extremely short-lived end stage of just a few thousand years before exploding, with the WC phase corresponding to the core helium burning phase and the WO phase to nuclear burning stages beyond. It is still unclear whether the WO spectrum is purely the result of ionisation effects at very high temperature, reflects an actual chemical abundance difference, or if both effects occur to varying degrees.
|Initial Mass (M☉)||Evolutionary Sequence||Supernova Type|
|60+||O → Of → WNh ↔ LBV →[WNL]||IIn|
|45–60||O → WNh → LBV/WNE? → WO||Ib/c|
|20–45||O → RSG → WNE → WC||Ib|
|15–20||O → RSG ↔ (YHG) ↔ BSG (blue loops)||II-L (or IIb)|
|8–15||B → RSG||II-P|
- O: O-type main-sequence star
- Of: evolved O-type showing N and He emission
- BSG: blue supergiant
- RSG: red supergiant
- YHG: yellow hypergiant
- LBV: luminous blue variable
- WNh: WN plus hydrogen lines
- WNL: "late" WN-class Wolf–Rayet star (about WN6 to WN9)
- WNE: "early" WN-class Wolf–Rayet star (about WN2 to WN6)
- WC: WC-class Wolf–Rayet star
- WO: WO-class Wolf–Rayet star
Wolf–Rayet stars form from massive stars, although the evolved population I stars have lost half or more of their initial masses by the time they show an WR appearance. For example, γ2 Velorum A currently has a mass around 9 times the sun, but began with a mass at least 40 times the sun. High-mass stars are very rare, both because they form less often and because they have short lives. This means that Wolf–Rayet stars themselves are extremely rare because they only form from the most massive main sequence stars and because they are a relatively short-lived phase in the lives of those stars. This also explains why type Ibc supernovae are less common than type II, since they result from higher mass stars.
WNh stars, spectroscopically similar but actually a much less evolved star which has only just started to expel its atmosphere, are an exception and still retain much of their initial mass. The most massive stars currently known are all WNh stars rather than O-type main sequence stars, an expected situation because such stars show helium and nitrogen at the surface only a few thousand years after they form, possibly before they become visible through the surrounding gas cloud. An alternative explanation is that these stars are so massive that they could not form as normal main sequence stars, instead being the result of mergers of less extreme stars.
The difficulties of modelling the observed numbers and types of Wolf Rayet stars through single star evolution have led to theories that they form through binary interactions which could accelerate loss of the outer layers of a star through mass exchange. WR 122 is a potential example that has a flat disk of gas encircling the star, almost 2 trillion miles wide, and may have a companion star that stripped its outer envelope.
Although it is widely accepted that most or all type Ibc supernovae progenitors were WR stars, no conclusive identification has been made of such a progenitor. WR stars are very luminous due to their high temperatures but not visually bright, especially the hottest examples that are expected to be supernova progenitors. Theory suggests that the progenitors of type Ibc supernovae observed to date would not be bright enough to be detected, although they place constraints on the properties of those progenitors. One candidate is under observation as pre-outburst observations show a likely WR star at the site of iPTF13bvn.
Particularly massive WR stars may produce a super-luminous type Ib/c supernova (hypernova) due to the high mass of radioactive nickel ejected. It is possible for a Wolf–Rayet star to progress to a "collapsar" stage in its death throes if it doesn't lose sufficient mass. This is when the core of the star collapses to form a black hole, either directly or by pulling in the surrounding ejected material. This is thought to be the precursor of a long gamma-ray burst. The compact object of Cygnus X-1 is one possible example.
The most visible example of a Wolf–Rayet star is Gamma 2 Velorum (γ² Vel), which is a naked eye star for those located south of 40 degrees northern latitude. Due to the exotic nature of its spectrum (bright emission lines in lieu of dark absorption lines) it is dubbed the "Spectral Gem of the Southern Skies". The second brightest is Theta Muscae. Both are multiple stars where the primary component is a Wolf Rayet type.
The most massive star and probably most luminous star currently known, R136a1, is also a Wolf–Rayet star of the WNh type that is still fusing hydrogen in its core. This type of star, which includes many of the most luminous and most massive stars, is very young and usually found only in the centre of the densest star clusters. Occasionally a runaway Wolf–Rayet star such as VFTS 682 is found outside such clusters, probably having been ejected from a multiple system or by interaction with other stars.
Only a minority of planetary nebulae have WR type central stars, but a considerable number of well-known planetary nebulae do have them.
|Planetary nebula||Central star type|
|NGC 5189 (Spiral Planetary Nebula)||[WO1]|
|NGC 6369 (Little Ghost Nebula)||[WO3]|
|MyCn18 (Hourglass Nebula)||[WC]-PG1159|
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