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{{short description|Class of star}}
{{short description|Class of massive star with a spectral type of A to K}}
[[Image:HR-vartype.svg|right|upright=1.35|thumb|Intrinsic variable types in the [[Hertzsprung–Russell diagram]] showing the Yellow Hypergiants above (i.e. more luminous than) the Cepheid [[instability strip]]]]
[[Image:HR-vartype.svg|right|upright=1.35|thumb|Intrinsic variable types in the [[Hertzsprung–Russell diagram]] showing the Yellow Hypergiants above (i.e. more luminous than) the Cepheid [[instability strip]]]]


A '''yellow hypergiant''' ('''YHG''') is a massive [[star]] with an extended [[atmosphere]], a [[spectral class]] from A to K, and, starting with an initial mass of about 20–60 [[solar masses]], has lost as much as half that mass. They are amongst the most visually luminous stars, with [[absolute magnitude]] (M<sub>V</sub>) around −9, but also one of the rarest, with just 15 known in the [[Milky Way]] and six of those in just [[Westerlund 1|a single cluster]]. They are sometimes referred to as cool [[hypergiant]]s in comparison with O- and B-type stars, and sometimes as warm hypergiants in comparison with red [[supergiant]]s.
A '''yellow hypergiant''' ('''YHG''') is a massive [[star]] with an extended [[atmosphere]], a [[spectral class]] from A to K, and, starting with an initial mass of about 20–60 [[solar masses]], has lost as much as half that mass. They are amongst the most visually luminous stars, with [[absolute magnitude]] (M<sub>V</sub>) around −9, but also one of the rarest, with just 20 known in the [[Milky Way]] and six of those in just [[Westerlund 1|a single cluster]]. They are sometimes referred to as cool [[hypergiant]]s in comparison with O- and B-type stars, and sometimes as warm hypergiants in comparison with red [[supergiant]]s.


==Classification==
==Classification==
The term "hypergiant" was used as early as 1929, but not for the stars currently known as hypergiants.<ref name=wallenquist>{{cite journal|bibcode=1929BAN.....5...67W|title=An attempt to determine the mean masses of the stars in the globular cluster M 3|journal=Bulletin of the Astronomical Institutes of the Netherlands|volume=5|pages=67|last1=Wallenquist|first1=Aå|year=1929}}</ref> Hypergiants are defined by their '0' [[luminosity class]], and are higher in luminosity than the brightest supergiants of class Ia,<ref>{{cite journal|bibcode=1943assw.book.....M|title=An atlas of stellar spectra, with an outline of spectral classification|journal=Chicago|last1=Morgan|first1=William Wilson|last2=Keenan|first2=Philip Childs|last3=Kellman|first3=Edith|year=1943}}</ref> although they were not referred to as hypergiants until the late 1970s.<ref name="dejager1980">{{cite book|doi=10.1007/978-94-009-9030-2_2|chapter=The Main Observational Characteristics of the Most Luminous Stars|title=The Brightest Stars|pages=18–56|year=1980|last1=De Jager|first1=Cornelis|isbn=978-90-277-1110-6}}</ref> Another criterion for hypergiants was also suggested in 1979 for some other highly luminous mass-losing hot stars,<ref name=desandres>{{cite journal|bibcode=1979A&AS...38..367L|title=Line Blocking in the Near Ultraviolet Spectrum of Early-Type Stars—Part Two—the Dependence on Spectral Type and Luminosity for Normal Stars|journal=Astronomy and Astrophysics Supplement|volume=38|pages=367|last1=Llorente De Andres|first1=F.|last2=Lamers|first2=H. J. G. L. M.|last3=Muller|first3=E. A.|year=1979}}</ref> but was not applied to cooler stars. In 1991, [[Rho Cassiopeiae]] was the first to be described as a yellow hypergiant,<ref name=zsoldos>{{cite journal|bibcode=1991A&A...246..441Z|title=Photometry of yellow semiregular variables - Rho Cassiopeiae|journal=Astronomy and Astrophysics |issn=0004-6361|volume=246|pages=441|last1=Zsoldos|first1=E.|last2=Percy|first2=J. R.|year=1991}}</ref> likely becoming grouped as a new class of luminous stars during discussions at the ''Solar physics and astrophysics at interferometric resolution'' workshop in 1992.<ref name=dejager>{{cite journal|bibcode=1992ESASP.344..109D|title=Yellow hypergiant interferometry: A clue to understanding evolutionary instability|journal=In ESA|volume=344|pages=109|last1=De Jager|first1=Cornelis|last2=Nieuwenhuijzen|first2=Hans|year=1992}}</ref>
The term "hypergiant" was used as early as 1929, but not for the stars currently known as hypergiants.<ref name=wallenquist>{{cite journal|bibcode=1929BAN.....5...67W|title=An attempt to determine the mean masses of the stars in the globular cluster M 3|journal=Bulletin of the Astronomical Institutes of the Netherlands|volume=5|pages=67|last1=Wallenquist|first1=Aå|year=1929}}</ref> Hypergiants are defined by their '0' [[luminosity class]], and are higher in luminosity than the brightest supergiants of class Ia,<ref>{{cite journal|bibcode=1943assw.book.....M|title=An atlas of stellar spectra, with an outline of spectral classification|journal=Chicago|last1=Morgan|first1=William Wilson|last2=Keenan|first2=Philip Childs|last3=Kellman|first3=Edith|year=1943}}</ref> although they were not referred to as hypergiants until the late 1970s.<ref name="dejager1980">{{cite book|doi=10.1007/978-94-009-9030-2_2|chapter=The Main Observational Characteristics of the Most Luminous Stars|title=The Brightest Stars|pages=18–56|year=1980|last1=De Jager|first1=Cornelis|isbn=978-90-277-1110-6}}</ref> Another criterion for hypergiants was also suggested in 1979 for some other highly luminous mass-losing hot stars,<ref name=desandres>{{cite journal|bibcode=1979A&AS...38..367L|title=Line Blocking in the Near Ultraviolet Spectrum of Early-Type Stars—Part Two—the Dependence on Spectral Type and Luminosity for Normal Stars|journal=Astronomy and Astrophysics Supplement|volume=38|pages=367|last1=Llorente De Andres|first1=F.|last2=Lamers|first2=H. J. G. L. M.|last3=Muller|first3=E. A.|year=1979}}</ref> but was not applied to cooler stars. In 1991, [[Rho Cassiopeiae]] was the first to be described as a yellow hypergiant,<ref name=zsoldos>{{cite journal|bibcode=1991A&A...246..441Z|title=Photometry of yellow semiregular variables - Rho Cassiopeiae|journal=Astronomy and Astrophysics |issn=0004-6361|volume=246|pages=441|last1=Zsoldos|first1=E.|last2=Percy|first2=J. R.|year=1991}}</ref> likely becoming grouped as a new class of luminous stars during discussions at the ''Solar physics and astrophysics at interferometric resolution'' workshop in 1992.<ref name=dejager>{{cite journal|bibcode=1992ESASP.344..109D|title=Yellow hypergiant interferometry: A clue to understanding evolutionary instability|journal=In ESA|volume=344|pages=109|last1=De Jager|first1=Cornelis|last2=Nieuwenhuijzen|first2=Hans|year=1992}}</ref>


Definitions of the term hypergiant remains vague, and although luminosity class 0 is for hypergiants, they are more commonly designated by the alternative luminosity classes Ia-0 and Ia<sup>+</sup>.<ref name=achmad>{{cite journal|bibcode=1992A&A...259..600A|title=A photometric study of the G0-4 Ia(+) hypergiant HD 96918 (V382 Carinae)|journal=Astronomy and Astrophysics |issn=0004-6361|volume=259|pages=600|last1=Achmad|first1=L.|last2=Lamers|first2=H. J. G. L. M.|last3=Nieuwenhuijzen|first3=H.|last4=Van Genderen|first4=A. M.|year=1992}}</ref> Their great stellar luminosities are determined from various spectral features, which are sensitive to surface gravity, such as Hβ line widths in hot stars or a strong [[Balmer discontinuity]] in cooler stars. Lower surface gravity often indicates larger stars, and hence, higher luminosities.<ref name=ubvy>{{cite journal|bibcode=1993A&A...268..653N|title=On the determination of effective temperature and surface gravity of B, A, and F stars using Stromgren UVBY beta photometry|journal=Astronomy and Astrophysics |issn=0004-6361|volume=268|pages=653|last1=Napiwotzki|first1=R.|last2=Schoenberner|first2=D.|last3=Wenske|first3=V.|year=1993}}</ref> In cooler stars, the strength of observed oxygen lines, such as O I at 777.4&nbsp;nm., can be used to calibrate directly against stellar luminosity.<ref name=ferro>{{cite journal|bibcode=2003RMxAA..39....3A|title=A Revised Calibration of the MV-W(O I 7774) Relationship using Hipparcos Data: Its Application to Cepheids and Evolved Stars|journal=Revista Mexicana de Astronomía y Astrofísica |volume=39|pages=3|last1=Arellano Ferro|first1=A.|last2=Giridhar|first2=S.|last3=Rojo Arellano|first3=E.|year=2003|arxiv = astro-ph/0210695}}</ref>
Definitions of the term hypergiant remain vague, and although luminosity class 0 is for hypergiants, they are more commonly designated by the alternative luminosity classes Ia-0 and Ia<sup>+</sup>.<ref name=achmad>{{cite journal|bibcode=1992A&A...259..600A|title=A photometric study of the G0-4 Ia(+) hypergiant HD 96918 (V382 Carinae)|journal=Astronomy and Astrophysics |issn=0004-6361|volume=259|pages=600|last1=Achmad|first1=L.|last2=Lamers|first2=H. J. G. L. M.|last3=Nieuwenhuijzen|first3=H.|last4=Van Genderen|first4=A. M.|year=1992}}</ref> Their great stellar luminosities are determined from various spectral features, which are sensitive to surface gravity, such as Hβ line widths in hot stars or a strong [[Balmer discontinuity]] in cooler stars. Lower surface gravity often indicates larger stars, and hence, higher luminosities.<ref name=ubvy>{{cite journal|bibcode=1993A&A...268..653N|title=On the determination of effective temperature and surface gravity of B, A, and F stars using Stromgren UVBY beta photometry|journal=Astronomy and Astrophysics |issn=0004-6361|volume=268|pages=653|last1=Napiwotzki|first1=R.|last2=Schoenberner|first2=D.|last3=Wenske|first3=V.|year=1993}}</ref> In cooler stars, the strength of observed oxygen lines, such as O I at 777.4&nbsp;nm., can be used to calibrate directly against stellar luminosity.<ref name=ferro>{{cite journal|bibcode=2003RMxAA..39....3A|title=A Revised Calibration of the MV-W(O I 7774) Relationship using Hipparcos Data: Its Application to Cepheids and Evolved Stars|journal=Revista Mexicana de Astronomía y Astrofísica |volume=39|pages=3|last1=Arellano Ferro|first1=A.|last2=Giridhar|first2=S.|last3=Rojo Arellano|first3=E.|year=2003|arxiv = astro-ph/0210695}}</ref>


One astrophysical method used to definitively identify yellow hypergiants is the so-called ''Keenan-Smolinski'' criterion. Here all absorption lines should be strongly broadened, beyond those expected of [[bright supergiant]] stars, and also show strong evidence of significant mass loss. Furthermore, at least one broadened [[H-alpha|Hα]] component should also be present. They may also display very complex Hα profiles, typically having strong emission lines combined with absorption lines.<ref name=dejaeger/>
One astrophysical method used to definitively identify yellow hypergiants is the so-called ''Keenan-Smolinski'' criterion. Here all absorption lines should be strongly broadened, beyond those expected of [[bright supergiant]] stars, and also show strong evidence of significant mass loss. Furthermore, at least one broadened [[H-alpha|Hα]] component should also be present. They may also display very complex Hα profiles, typically having strong emission lines combined with absorption lines.<ref name=dejaeger/>


The terminology of yellow hypergiants is further complicated by referring to them as either cool hypergiants or warm hypergiants, depending on the context. Cool hypergiants refers to all sufficiently luminous and unstable stars cooler than blue hypergiants and [[Luminous blue variable|LBV]]s, including both yellow and red hypergiants.<ref name=cool>{{cite journal|bibcode=2013ASPC..470..167L|title=Long-term Spectroscopic Monitoring of Cool Hypergiants HR 8752, IRC+10420, and 6 Cas near the Yellow Evolutionary Void|journal=370 Years of Astronomy in Utrecht. Proceedings of a Conference Held 2–5 April|volume=470|pages=167|last1=Lobel|first1=A.|last2=De Jager|first2=K.|last3=Nieuwenhuijzen|first3=H.|date=2013}}</ref> The term warm hypergiants has been used for highly luminous class A and F stars in M31 and M33 that are not LBVs,<ref name=warm>{{Cite journal|arxiv=1305.6051|last1= Humphreys|first1= Roberta M.|title= Luminous and Variable Stars in M31 and M33. I. The Warm Hypergiants and Post-Red Supergiant Evolution|journal= The Astrophysical Journal|volume= 773|issue= 1|pages= 46|last2= Davidson|first2= Kris|last3= Grammer|first3= Skyler|last4= Kneeland|first4= Nathan|last5= Martin|first5= John C.|last6= Weis|first6= Kerstin|last7= Burggraf|first7= Birgitta|date= 2013|doi= 10.1088/0004-637X/773/1/46|bibcode= 2013ApJ...773...46H|s2cid= 118413197}}</ref> as well as more generally for yellow hypergiants.<ref name=shenov>{{cite journal|bibcode=2016AJ....151...51S|arxiv=1512.01529|title=Searching for Cool Dust in the Mid-to-far Infrared: The Mass-loss Histories of the Hypergiants μ Cep, VY CMa, IRC+10420, and ρ Cas|journal=The Astronomical Journal|volume=151|issue=3|pages=51|last1=Shenoy|first1=Dinesh|last2=Humphreys|first2=Roberta M.|last3=Jones|first3=Terry J.|last4=Marengo|first4=Massimo|last5=Gehrz|first5=Robert D.|last6=Helton|first6=L. Andrew|last7=Hoffmann|first7=William F.|last8=Skemer|first8=Andrew J.|last9=Hinz|first9=Philip M.|year=2016|doi=10.3847/0004-6256/151/3/51|s2cid=119281306}}</ref>
The terminology of yellow hypergiants is further complicated by referring to them as either cool hypergiants or warm hypergiants, depending on the context. Cool hypergiants refers to all sufficiently luminous and unstable stars cooler than blue hypergiants and [[Luminous blue variable|LBV]]s, including both yellow and red hypergiants.<ref name=cool>{{cite journal|bibcode=2013ASPC..470..167L|title=Long-term Spectroscopic Monitoring of Cool Hypergiants HR 8752, IRC+10420, and 6 Cas near the Yellow Evolutionary Void|journal=370 Years of Astronomy in Utrecht. Proceedings of a Conference Held 2–5 April|volume=470|pages=167|last1=Lobel|first1=A.|last2=De Jager|first2=K.|last3=Nieuwenhuijzen|first3=H.|date=2013}}</ref> The term warm hypergiants has been used for highly luminous class A and F stars in M31 and M33 that are not LBVs,<ref name=warm>{{Cite journal|arxiv=1305.6051|last1= Humphreys|first1= Roberta M.|title= Luminous and Variable Stars in M31 and M33. I. The Warm Hypergiants and Post-Red Supergiant Evolution|journal= The Astrophysical Journal|volume= 773|issue= 1|pages= 46|last2= Davidson|first2= Kris|last3= Grammer|first3= Skyler|last4= Kneeland|first4= Nathan|last5= Martin|first5= John C.|last6= Weis|first6= Kerstin|last7= Burggraf|first7= Birgitta|date= 2013|doi= 10.1088/0004-637X/773/1/46|bibcode= 2013ApJ...773...46H|s2cid= 118413197}}</ref> as well as more generally for yellow hypergiants.<ref name=shenov>{{cite journal|bibcode=2016AJ....151...51S|arxiv=1512.01529|title=Searching for Cool Dust in the Mid-to-far Infrared: The Mass-loss Histories of the Hypergiants μ Cep, VY CMa, IRC+10420, and ρ Cas|journal=The Astronomical Journal|volume=151|issue=3|pages=51|last1=Shenoy|first1=Dinesh|last2=Humphreys|first2=Roberta M.|last3=Jones|first3=Terry J.|last4=Marengo|first4=Massimo|last5=Gehrz|first5=Robert D.|last6=Helton|first6=L. Andrew|last7=Hoffmann|first7=William F.|last8=Skemer|first8=Andrew J.|last9=Hinz|first9=Philip M.|year=2016|doi=10.3847/0004-6256/151/3/51|s2cid=119281306 |doi-access=free }}</ref>


==Characteristics==
==Characteristics==
[[File:Rhocas lightcurve.png|thumb|left|Visual light curve for [[ρ Cassiopeiae]] from 1933 to 2015]]
[[File:Rhocas lightcurve.png|thumb|left|Visual light curve for [[ρ Cassiopeiae]] from 1933 to 2015]]
Yellow hypergiants occupy a region of the [[Hertzsprung–Russell diagram]] above the [[instability strip]], a region where relatively few stars are found and where those stars are generally unstable. The spectral and temperature ranges are approximately A0-K2 and 4,000–8,000K respectively. The area is bounded on the high-temperature side by the ''Yellow Evolutionary Void'' where stars of this luminosity become extremely unstable and experience severe mass loss. The “Yellow Evolutionary Void” separates yellow hypergiants from [[luminous blue variable]]s although yellow hypergiants at their hottest and luminous blue variables at their coolest can have approximately the same temperature near 8,000&nbsp;K. At the lower temperature bound, yellow hypergiants and red supergiants are not clearly separated; [[RW Cephei]] (roughly 4,000&nbsp;K, {{solar luminosity|link=y|295,000}}) is an example of a star that shares characteristics of both yellow hypergiants and red supergiants.<ref name=stothers/><ref name=void/>
Yellow hypergiants occupy a region of the [[Hertzsprung–Russell diagram]] above the [[instability strip]], a region where relatively few stars are found and where those stars are generally unstable. The spectral and temperature ranges are approximately A0-K2 and {{convert|4000–8000|K|C F|abbr=on}} respectively. The area is bounded on the high-temperature side by the ''Yellow Evolutionary Void'' where stars of this luminosity become extremely unstable and experience severe mass loss. The “Yellow Evolutionary Void” separates yellow hypergiants from [[luminous blue variable]]s although yellow hypergiants at their hottest and luminous blue variables at their coolest can have approximately the same temperature near 8,000&nbsp;K. At the lower temperature bound, yellow hypergiants and red supergiants are not clearly separated; [[RW Cephei]] (roughly {{convert|4000|K|C F|abbr=on}}, {{solar luminosity|link=y|295,000}}) is an example of a star that shares characteristics of both yellow hypergiants and red supergiants.<ref name=stothers/><ref name=void/>


Yellow hypergiants have a fairly narrow range of luminosities above {{solar luminosity|200,000}} (e.g. [[V382 Carinae]] at {{solar luminosity|212,000}}) and below the Humphrey-Davidson limit at around {{solar luminosity|600,000}}. With their output peaking in the middle of the visual range, these are the most visually bright stars known with absolute magnitudes around −9 or −9.5&nbsp;.<ref name=zsoldos/>
Yellow hypergiants have a fairly narrow range of luminosities above {{solar luminosity|200,000}} (e.g. [[V382 Carinae]] at {{solar luminosity|212,000}}) and below the Humphrey-Davidson limit at around {{solar luminosity|600,000}}. With their output peaking in the middle of the visual range, these are the most visually bright stars known with absolute magnitudes around −9 or −9.5&nbsp;.<ref name=zsoldos/>


They are large and somewhat unstable, with very low surface gravities. Where [[yellow supergiant]]s have surface gravities (log&nbsp;g) below about&nbsp;2, the yellow hypergiants have log&nbsp;g around zero. In addition they pulsate irregularly, producing small variations in temperature and brightness. This produces very high mass loss rates, and nebulosity is common around the stars.<ref name=rhocas>{{cite journal |last1= Lobel |first1= A. |last2= Israelian |first2= G. |last3= de Jager |first3= C. |last4= Musaev |first4= F. |last5= Parker |first5= J. W. |last6= Mavrogiorgou |first6= A. |title= The spectral variability of the cool hypergiant rho Cassiopeiae |journal= Astronomy and Astrophysics |date= 1998 |volume= 330 |pages= 659–675 |bibcode= 1998A&A...330..659L }}</ref> Occasional larger outbursts can temporarily obscure the stars.<ref name=outburst>{{cite journal |bibcode=2004IAUS..219..903L |author1=Lobel |author2=Stefanik |author3=Torres |author4=Davis |author5=Ilyin |author6=Rosenbush |title=Spectroscopy of the Millennium Outburst and Recent Variability of the Yellow Hypergiant Rho Cassiopeiae |journal=Stars as Suns : Activity |volume=219 |pages=903 |date=2003 |arxiv = astro-ph/0312074 }}</ref>
They are large and somewhat unstable, with very low surface gravities. Where [[yellow supergiant]]s have surface gravities (log&nbsp;g) below about&nbsp;2, the yellow hypergiants have log&nbsp;g around zero. In addition they pulsate irregularly, producing small variations in temperature and brightness. This produces very high mass loss rates, and nebulosity is common around the stars.<ref name=rhocas>{{cite journal |last1= Lobel |first1= A. |last2= Israelian |first2= G. |last3= de Jager |first3= C. |last4= Musaev |first4= F. |last5= Parker |first5= J. W. |last6= Mavrogiorgou |first6= A. |title= The spectral variability of the cool hypergiant rho Cassiopeiae |journal= Astronomy and Astrophysics |date= 1998 |volume= 330 |pages= 659–675 |bibcode= 1998A&A...330..659L }}</ref> Occasional larger outbursts can temporarily obscure the stars.<ref name=outburst>{{cite journal |bibcode=2004IAUS..219..903L |author1=Lobel |author2=Stefanik |author3=Torres |author4=Davis |author5=Ilyin |author6=Rosenbush |title=Spectroscopy of the Millennium Outburst and Recent Variability of the Yellow Hypergiant Rho Cassiopeiae |journal=Stars as Suns: Activity |volume=219 |pages=903 |date=2003 |arxiv = astro-ph/0312074 }}</ref>


Yellow hypergiants form from massive stars after they have evolved away from the main sequence. Most observed yellow hypergiants have been through a red supergiant phase and are evolving back towards higher temperatures, but a few are seen in the brief first transition from main sequence to red supergiant. Supergiants with an initial mass less than {{solar mass|20}} will explode as a supernova while still red supergiants, while stars more massive than about {{solar mass|60}} will never cool beyond blue supergiant temperatures. The exact mass ranges depend on [[metallicity]] and rotation.<ref name=groh2013>{{cite journal|bibcode=2013A&A...558A.131G|arxiv=1308.4681|title=Fundamental properties of core-collapse supernova and GRB progenitors: Predicting the look of massive stars before death|journal=Astronomy & Astrophysics|volume=558|pages=A131|last1=Groh|first1=Jose H.|last2=Meynet|first2=Georges|last3=Georgy|first3=Cyril|last4=Ekström|first4=Sylvia|year=2013|doi=10.1051/0004-6361/201321906|s2cid=84177572}}</ref> Yellow supergiants cooling for the first time may be massive stars of up to {{solar mass|60}} or more,<ref name=void/> but post-red supergiant stars will have lost around half their initial mass.<ref name=gesicki>{{cite journal|bibcode=1992A&A...254..280G|title=A Modelling of Circumstellar BAII Lines for the Hypergiant Rho-Cassiopeiae|journal=Astronomy and Astrophysics|volume=254|pages=280|last1=Gesicki|first1=K.|date=1992}}</ref>
Yellow hypergiants form from massive stars after they have evolved away from the main sequence. Most observed yellow hypergiants have been through a red supergiant phase and are evolving back towards higher temperatures, but a few are seen in the brief first transition from main sequence to red supergiant. Supergiants with an initial mass less than {{solar mass|20}} will explode as a supernova while still red supergiants, while stars more massive than about {{solar mass|60}} will never cool beyond blue supergiant temperatures. The exact mass ranges depend on [[metallicity]] and rotation.<ref name=groh2013>{{cite journal|bibcode=2013A&A...558A.131G|arxiv=1308.4681|title=Fundamental properties of core-collapse supernova and GRB progenitors: Predicting the look of massive stars before death|journal=Astronomy & Astrophysics|volume=558|pages=A131|last1=Groh|first1=Jose H.|last2=Meynet|first2=Georges|last3=Georgy|first3=Cyril|last4=Ekström|first4=Sylvia|year=2013|doi=10.1051/0004-6361/201321906|s2cid=84177572}}</ref> Yellow supergiants cooling for the first time may be massive stars of up to {{solar mass|60}} or more,<ref name=void/> but post-red supergiant stars will have lost around half their initial mass.<ref name=gesicki>{{cite journal|bibcode=1992A&A...254..280G|title=A Modelling of Circumstellar BAII Lines for the Hypergiant Rho-Cassiopeiae|journal=Astronomy and Astrophysics|volume=254|pages=280|last1=Gesicki|first1=K.|date=1992}}</ref>
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==Evolution==
==Evolution==
Yellow hypergiants have clearly evolved off the main sequence and so have depleted the hydrogen in their cores. The majority of yellow hypergiants are postulated to be post-[[red supergiant]]s evolving blueward,<ref name=stothers>{{Cite journal | last1 = Stothers | first1 = R. B. | last2 = Chin | first2 = C. W. | doi = 10.1086/322438 | title = Yellow Hypergiants as Dynamically Unstable Post–Red Supergiant Stars | journal = The Astrophysical Journal | volume = 560 | issue = 2 | pages = 934 | year = 2001 |bibcode = 2001ApJ...560..934S | doi-access = free }}</ref> while more stable and less luminous yellow supergiants are likely to be evolving to red supergiants for the first time. There is strong chemical and surface gravity evidence that the brightest of the yellow supergiants, [[HD 33579]], is currently expanding from a blue supergiant to a red supergiant.<ref name=void>{{cite journal | last1 = Nieuwenhuijzen | first1 = H | last2 = de Jager | first2 = C | title = Checking the yellow evolutionary void. Three evolutionary critical Hypergiants: HD 33579, HR 8752 & IRC +10420 | journal = Astronomy and Astrophysics | date = 2000 | volume = 353 | pages = 163–176 |bibcode = 2000A&A...353..163N }}</ref>
Yellow hypergiants have clearly evolved off the main sequence and so have depleted the hydrogen in their cores. The majority of yellow hypergiants are postulated to be post-[[red supergiant]]s evolving blueward,<ref name=stothers>{{Cite journal | last1 = Stothers | first1 = R. B. | last2 = Chin | first2 = C. W. | doi = 10.1086/322438 | title = Yellow Hypergiants as Dynamically Unstable Post–Red Supergiant Stars | journal = The Astrophysical Journal | volume = 560 | issue = 2 | pages = 934 | year = 2001 |bibcode = 2001ApJ...560..934S | doi-access = free | hdl = 2060/20010083764 | hdl-access = free }}</ref> while more stable and less luminous yellow supergiants are likely to be evolving to red supergiants for the first time. There is strong chemical and surface gravity evidence that the brightest of the yellow supergiants, [[HD 33579]], is currently expanding from a blue supergiant to a red supergiant.<ref name=void>{{cite journal | last1 = Nieuwenhuijzen | first1 = H | last2 = de Jager | first2 = C | title = Checking the yellow evolutionary void. Three evolutionary critical Hypergiants: HD 33579, HR 8752 & IRC +10420 | journal = Astronomy and Astrophysics | date = 2000 | volume = 353 | pages = 163–176 |bibcode = 2000A&A...353..163N }}</ref>


These stars are doubly rare because they are very massive, initially hot class O-type main-sequence stars more than 15 times as massive as the Sun, but also because they spend only a few thousand years in the unstable yellow void phase of their lives. In fact, it is difficult to explain even the small number of observed yellow hypergiants, relative to red supergiants of comparable luminosity, from simple models of stellar evolution. The most luminous red supergiants may execute multiple "blue loops", shedding much of their atmosphere, but without actually ever reaching the blue supergiant stage, each one taking only a few decades at most. Conversely, some apparent yellow hypergiants may be hotter stars, such as the "missing" LBVs, masked within a cool pseudo-photosphere.<ref name=stothers/>
These stars are doubly rare because they are very massive, initially hot class O-type main-sequence stars more than 15 times as massive as the Sun, but also because they spend only a few thousand years in the unstable yellow void phase of their lives. In fact, it is difficult to explain even the small number of observed yellow hypergiants, relative to red supergiants of comparable luminosity, from simple models of stellar evolution. The most luminous red supergiants may execute multiple "blue loops", shedding much of their atmosphere, but without actually ever reaching the blue supergiant stage, each one taking only a few decades at most. Conversely, some apparent yellow hypergiants may be hotter stars, such as the "missing" LBVs, masked within a cool pseudo-photosphere.<ref name=stothers/>


Recent discoveries of blue supergiant supernova progenitors have also raised the question of whether stars could explode directly from the yellow hypergiant stage.<ref name=supernova>{{Cite journal | last1 = Langer | first1 = N. | last2 = Norman | first2 = C. A. | last3 = De Koter | first3 = A. | last4 = Vink | first4 = J. S. | last5 = Cantiello | first5 = M. | last6 = Yoon | first6 = S. -C. | doi = 10.1051/0004-6361:20078482 | title = Pair creation supernovae at low and high redshift | journal = Astronomy and Astrophysics | volume = 475 | issue = 2 | pages = L19 | year = 2007 |arxiv = 0708.1970 |bibcode = 2007A&A...475L..19L | s2cid = 53516453 }}</ref> A handful of possible yellow supergiant supernova progenitors have been discovered, but they all appear to be of relatively low mass and luminosity, not hypergiants.<ref name=progenitors>{{Cite journal | last1 = Georgy | first1 = C. | doi = 10.1051/0004-6361/201118372 | title = Yellow supergiants as supernova progenitors: An indication of strong mass loss for red supergiants? | journal = Astronomy & Astrophysics | volume = 538 | pages = L8–L2 | year = 2012 |arxiv = 1111.7003 |bibcode = 2012A&A...538L...8G | s2cid = 55001976 }}</ref><ref name=20011dh>{{Cite journal | last1 = Maund | first1 = J. R. | last2 = Fraser | first2 = M. | last3 = Ergon | first3 = M. | last4 = Pastorello | first4 = A. | last5 = Smartt | first5 = S. J. | last6 = Sollerman | first6 = J. | last7 = Benetti | first7 = S. | last8 = Botticella | first8 = M. -T. | last9 = Bufano | first9 = F. | last10 = Danziger | doi = 10.1088/2041-8205/739/2/L37 | first10 = I. J. | last11 = Kotak | first11 = R. | last12 = Magill | first12 = L. | last13 = Stephens | first13 = A. W. | last14 = Valenti | first14 = S. | title = The Yellow Supergiant Progenitor of the Type II Supernova 2011dh in M51| journal = The Astrophysical Journal | volume = 739 | issue = 2 | pages = L37 | year = 2011 |arxiv = 1106.2565 |bibcode = 2011ApJ...739L..37M | s2cid = 118993104 }}</ref> [[SN 2013cu]] is a type IIb supernova whose progenitor has been directly and clearly observed. It was an evolved star around 8,000K showing extreme mass loss of helium and nitrogen enriched material. Although the luminosity is not known, only a yellow hypergiant or luminous blue variable in outburst would have these properties.<ref>{{cite journal|doi = 10.1051/0004-6361/201424852|journal = Astronomy & Astrophysics|volume = 572|pages = L11|year = 2014|last1 = Groh|first1 = Jose H.|title = Early-time spectra of supernovae and their precursor winds|bibcode = 2014A&A...572L..11G|arxiv = 1408.5397 |s2cid = 118935040}}</ref>
Recent discoveries of blue supergiant supernova progenitors have also raised the question of whether stars could explode directly from the yellow hypergiant stage.<ref name=supernova>{{Cite journal | last1 = Langer | first1 = N. | last2 = Norman | first2 = C. A. | last3 = De Koter | first3 = A. | last4 = Vink | first4 = J. S. | last5 = Cantiello | first5 = M. | last6 = Yoon | first6 = S. -C. | doi = 10.1051/0004-6361:20078482 | title = Pair creation supernovae at low and high redshift | journal = Astronomy and Astrophysics | volume = 475 | issue = 2 | pages = L19 | year = 2007 |arxiv = 0708.1970 |bibcode = 2007A&A...475L..19L | s2cid = 53516453 }}</ref> A handful of possible yellow supergiant supernova progenitors have been discovered, but they all appear to be of relatively low mass and luminosity, not hypergiants.<ref name=progenitors>{{Cite journal | last1 = Georgy | first1 = C. | doi = 10.1051/0004-6361/201118372 | title = Yellow supergiants as supernova progenitors: An indication of strong mass loss for red supergiants? | journal = Astronomy & Astrophysics | volume = 538 | pages = L8–L2 | year = 2012 |arxiv = 1111.7003 |bibcode = 2012A&A...538L...8G | s2cid = 55001976 }}</ref><ref name=20011dh>{{Cite journal | last1 = Maund | first1 = J. R. | last2 = Fraser | first2 = M. | last3 = Ergon | first3 = M. | last4 = Pastorello | first4 = A. | last5 = Smartt | first5 = S. J. | last6 = Sollerman | first6 = J. | last7 = Benetti | first7 = S. | last8 = Botticella | first8 = M. -T. | last9 = Bufano | first9 = F. | last10 = Danziger | doi = 10.1088/2041-8205/739/2/L37 | first10 = I. J. | last11 = Kotak | first11 = R. | last12 = Magill | first12 = L. | last13 = Stephens | first13 = A. W. | last14 = Valenti | first14 = S. | title = The Yellow Supergiant Progenitor of the Type II Supernova 2011dh in M51| journal = The Astrophysical Journal | volume = 739 | issue = 2 | pages = L37 | year = 2011 |arxiv = 1106.2565 |bibcode = 2011ApJ...739L..37M | s2cid = 118993104 }}</ref> [[SN 2013cu]] is a type IIb supernova whose progenitor has been directly and clearly observed. It was an evolved star around {{convert|8000|K|C F|abbr=on}} showing extreme mass loss of helium and nitrogen enriched material. Although the luminosity is not known, only a yellow hypergiant or luminous blue variable in outburst would have these properties.<ref>{{cite journal|doi = 10.1051/0004-6361/201424852|journal = Astronomy & Astrophysics|volume = 572|pages = L11|year = 2014|last1 = Groh|first1 = Jose H.|title = Early-time spectra of supernovae and their precursor winds|bibcode = 2014A&A...572L..11G|arxiv = 1408.5397 |s2cid = 118935040}}</ref>


Modern models suggest that stars with a certain range of masses and rotation rates may explode as [[supernovae]] without ever becoming blue supergiants again, but many will eventually pass right through the yellow void and become low-mass low-luminosity [[luminous blue variable]]s and possibly [[Wolf–Rayet star]]s after that.<ref name=lbv>{{Cite journal | last1 = Smith | first1 = N. | last2 = Vink | first2 = J. S. | last3 = De Koter | first3 = A. | title = The Missing Luminous Blue Variables and the Bistability Jump | doi = 10.1086/424030 | journal = The Astrophysical Journal | volume = 615 | issue = 1 | pages = 475–484 | year = 2004 |arxiv = astro-ph/0407202 |bibcode = 2004ApJ...615..475S | s2cid = 17904692 }}</ref> Specifically, more massive stars and those with higher mass loss rates due to rotation or high metallicity will evolve beyond the yellow hypergiant stage to hotter temperatures before reaching core collapse.<ref name=chieffy>{{cite journal|doi=10.1088/0004-637X/764/1/21|title=Pre-Supernova Evolution of Rotating Solar Metallicity Stars in the Mass Range 13-120M☉And Their Explosive Yields|journal=The Astrophysical Journal|volume=764|issue=1|pages=21|year=2013|last1=Chieffi|first1=Alessandro|last2=Limongi|first2=Marco|bibcode=2013ApJ...764...21C|doi-access=free}}</ref>
Modern models suggest that stars with a certain range of masses and rotation rates may explode as [[supernovae]] without ever becoming blue supergiants again, but many will eventually pass right through the yellow void and become low-mass low-luminosity [[luminous blue variable]]s and possibly [[Wolf–Rayet star]]s after that.<ref name=lbv>{{Cite journal | last1 = Smith | first1 = N. | last2 = Vink | first2 = J. S. | last3 = De Koter | first3 = A. | title = The Missing Luminous Blue Variables and the Bistability Jump | doi = 10.1086/424030 | journal = The Astrophysical Journal | volume = 615 | issue = 1 | pages = 475–484 | year = 2004 |arxiv = astro-ph/0407202 |bibcode = 2004ApJ...615..475S | s2cid = 17904692 }}</ref> Specifically, more massive stars and those with higher mass loss rates due to rotation or high metallicity will evolve beyond the yellow hypergiant stage to hotter temperatures before reaching core collapse.<ref name=chieffy>{{cite journal|doi=10.1088/0004-637X/764/1/21|title=Pre-Supernova Evolution of Rotating Solar Metallicity Stars in the Mass Range 13-120M☉And Their Explosive Yields|journal=The Astrophysical Journal|volume=764|issue=1|pages=21|year=2013|last1=Chieffi|first1=Alessandro|last2=Limongi|first2=Marco|bibcode=2013ApJ...764...21C|doi-access=free}}</ref>
Line 38: Line 38:
According to the current physical models of stars, a yellow hypergiant should possess a [[convection|convective]] core surrounded by a [[radiation|radiative]] zone, as opposed to a sun-sized star, which consists of a radiative core surrounded by a [[convective zone]].<ref name=convection>{{Cite journal | last1 = Fadeyev | first1 = Y. A. | title = Pulsational instability of yellow hypergiants | doi = 10.1134/S1063773711060016 | journal = Astronomy Letters | volume = 37 | issue = 6 | pages = 403–413 | year = 2011 |arxiv = 1102.3810 |bibcode = 2011AstL...37..403F | s2cid = 118642288 }}</ref> Because of their extreme luminosity and internal structure,<ref name=structure>{{cite journal|bibcode=1998RvMA...11...57L|title=Massive Stars: The Pre-Supernova Evolution of Internal and Circumstellar Structure|journal=Reviews in Modern Astronomy 11: Stars and Galaxies|editor=Reinhard E. Schielicke |location=Hamburg|volume=11|pages=57|last1=Langer|first1=Norbert|last2=Heger|first2=Alexander|last3=García-Segura|first3=Guillermo|date=1998}}</ref> yellow hypergiants suffer high rates of mass loss<ref name=massloss>{{Cite journal | last1 = Dinh-v-Trung | last2 = Muller | first2 = S. B. | last3 = Lim | first3 = J. | last4 = Kwok | first4 = S. | last5 = Muthu | first5 = C. | title = Probing the Mass-Loss History of the Yellow Hypergiant IRC+10420 | doi = 10.1088/0004-637X/697/1/409 | journal = The Astrophysical Journal | volume = 697 | issue = 1 | pages = 409–419 | year = 2009 |arxiv = 0903.3714 |bibcode = 2009ApJ...697..409D | s2cid = 16971892 }}</ref> and are generally surrounded by envelopes of expelled material. An example of the nebulae that can result is [[IRAS 17163-3907]], known as the Fried Egg, which has expelled several solar masses of material in just a few hundred years.<ref name=egg>{{Cite journal | last1 = Lagadec | first1 = E. | last2 = Zijlstra | first2 = A. A. | last3 = Oudmaijer | first3 = R. D. | last4 = Verhoelst | first4 = T. | last5 = Cox | first5 = N. L. J. | last6 = Szczerba | first6 = R. | last7 = Mékarnia | first7 = D. | last8 = Van Winckel | first8 = H. | doi = 10.1051/0004-6361/201117521 | title = A double detached shell around a post-red supergiant: IRAS 17163-3907, the Fried Egg nebula | journal = Astronomy & Astrophysics | volume = 534 | pages = L10 | year = 2011 |arxiv = 1109.5947 |bibcode = 2011A&A...534L..10L | s2cid = 55754316 }}</ref>
According to the current physical models of stars, a yellow hypergiant should possess a [[convection|convective]] core surrounded by a [[radiation|radiative]] zone, as opposed to a sun-sized star, which consists of a radiative core surrounded by a [[convective zone]].<ref name=convection>{{Cite journal | last1 = Fadeyev | first1 = Y. A. | title = Pulsational instability of yellow hypergiants | doi = 10.1134/S1063773711060016 | journal = Astronomy Letters | volume = 37 | issue = 6 | pages = 403–413 | year = 2011 |arxiv = 1102.3810 |bibcode = 2011AstL...37..403F | s2cid = 118642288 }}</ref> Because of their extreme luminosity and internal structure,<ref name=structure>{{cite journal|bibcode=1998RvMA...11...57L|title=Massive Stars: The Pre-Supernova Evolution of Internal and Circumstellar Structure|journal=Reviews in Modern Astronomy 11: Stars and Galaxies|editor=Reinhard E. Schielicke |location=Hamburg|volume=11|pages=57|last1=Langer|first1=Norbert|last2=Heger|first2=Alexander|last3=García-Segura|first3=Guillermo|date=1998}}</ref> yellow hypergiants suffer high rates of mass loss<ref name=massloss>{{Cite journal | last1 = Dinh-v-Trung | last2 = Muller | first2 = S. B. | last3 = Lim | first3 = J. | last4 = Kwok | first4 = S. | last5 = Muthu | first5 = C. | title = Probing the Mass-Loss History of the Yellow Hypergiant IRC+10420 | doi = 10.1088/0004-637X/697/1/409 | journal = The Astrophysical Journal | volume = 697 | issue = 1 | pages = 409–419 | year = 2009 |arxiv = 0903.3714 |bibcode = 2009ApJ...697..409D | s2cid = 16971892 }}</ref> and are generally surrounded by envelopes of expelled material. An example of the nebulae that can result is [[IRAS 17163-3907]], known as the Fried Egg, which has expelled several solar masses of material in just a few hundred years.<ref name=egg>{{Cite journal | last1 = Lagadec | first1 = E. | last2 = Zijlstra | first2 = A. A. | last3 = Oudmaijer | first3 = R. D. | last4 = Verhoelst | first4 = T. | last5 = Cox | first5 = N. L. J. | last6 = Szczerba | first6 = R. | last7 = Mékarnia | first7 = D. | last8 = Van Winckel | first8 = H. | doi = 10.1051/0004-6361/201117521 | title = A double detached shell around a post-red supergiant: IRAS 17163-3907, the Fried Egg nebula | journal = Astronomy & Astrophysics | volume = 534 | pages = L10 | year = 2011 |arxiv = 1109.5947 |bibcode = 2011A&A...534L..10L | s2cid = 55754316 }}</ref>


The yellow hypergiant is an expected phase of evolution as the most luminous red supergiants evolve bluewards, but they may also represent a different sort of star. LBVs during eruption have such dense winds that they form a pseudo-photosphere which appears as a larger cooler star despite the underlying blue supergiant being largely unchanged. These are observed to have a very narrow range of temperatures around 8,000K. At the bistability jump which occurs around 21,000K blue supergiant winds become several times denser and could be result in an even cooler pseudo-photosphere. No LBVs are observed just below the luminosity where the bistability jump crosses the [[S Doradus variable|S Doradus instability strip]] (not to be confused with the [[instability strip|Cepheid instability strip]]), but it is theorised that they do exist and appear as yellow hypergiants because of their pseudo-photospheres.<ref name=pseudo>{{Cite journal | last1 = Benaglia | first1 = P. | last2 = Vink | first2 = J. S. | last3 = Martí | first3 = J. | last4 = Maíz Apellániz | first4 = J. | last5 = Koribalski | first5 = B. | last6 = Crowther | first6 = P. A. | doi = 10.1051/0004-6361:20077139 | title = Testing the predicted mass-loss bi-stability jump at radio wavelengths | journal = Astronomy and Astrophysics | volume = 467 | issue = 3 | pages = 1265 | year = 2007 |arxiv = astro-ph/0703577 |bibcode = 2007A&A...467.1265B | s2cid = 14601449 }}</ref>
The yellow hypergiant is an expected phase of evolution as the most luminous red supergiants evolve bluewards, but they may also represent a different sort of star. LBVs during eruption have such dense winds that they form a pseudo-photosphere which appears as a larger cooler star despite the underlying blue supergiant being largely unchanged. These are observed to have a very narrow range of temperatures around {{convert|8000|K|C F|abbr=on}}. At the bistability jump which occurs around {{convert|21000|K|C F|abbr=on}} blue supergiant winds become several times denser and could be result in an even cooler pseudo-photosphere. No LBVs are observed just below the luminosity where the bistability jump crosses the [[S Doradus variable|S Doradus instability strip]] (not to be confused with the [[instability strip|Cepheid instability strip]]), but it is theorised that they do exist and appear as yellow hypergiants because of their pseudo-photospheres.<ref name=pseudo>{{Cite journal | last1 = Benaglia | first1 = P. | last2 = Vink | first2 = J. S. | last3 = Martí | first3 = J. | last4 = Maíz Apellániz | first4 = J. | last5 = Koribalski | first5 = B. | last6 = Crowther | first6 = P. A. | doi = 10.1051/0004-6361:20077139 | title = Testing the predicted mass-loss bi-stability jump at radio wavelengths | journal = Astronomy and Astrophysics | volume = 467 | issue = 3 | pages = 1265 | year = 2007 |arxiv = astro-ph/0703577 |bibcode = 2007A&A...467.1265B | s2cid = 14601449 }}</ref>
{{clear}}
{{clear}}


Line 44: Line 44:
[[Image:The field around yellow hypergiant star HR 5171.jpg|thumb|right|Yellow hypergiant [[HR 5171]] A, seen as the bright yellow star at the center of the image.]]
[[Image:The field around yellow hypergiant star HR 5171.jpg|thumb|right|Yellow hypergiant [[HR 5171]] A, seen as the bright yellow star at the center of the image.]]
[[File:Artist’s impression of the yellow hypergiant star HR 5171.ogv|thumb|right|Artist's impression of the binary system containing yellow hypergiant [[HR 5171]] A]]
[[File:Artist’s impression of the yellow hypergiant star HR 5171.ogv|thumb|right|Artist's impression of the binary system containing yellow hypergiant [[HR 5171]] A]]
===In Milky Way galaxy ===

* [[Rho Cassiopeiae]]
* [[Rho Cassiopeiae]]
* [[V509 Cassiopeiae]]
* [[V509 Cassiopeiae]]
* [[Omicron1 Centauri]]<ref>{{Cite journal |last1=Keenan |first1=P. C. |last2=Pitts |first2=R. E. |date=1980-04-01 |title=Revised MK spectral types for G, K ANS M stars. |journal=The Astrophysical Journal Supplement Series |volume=42 |pages=541–563 |doi=10.1086/190662 |issn=0067-0049|doi-access=free |bibcode=1980ApJS...42..541K }}</ref>
* [[R Puppis]]<ref name="keenan">{{Cite journal | last1 = Keenan | first1 = P. C. | last2 = McNeil | first2 = R. C. | doi = 10.1086/191373 | title = The Perkins catalog of revised MK types for the cooler stars | journal = The Astrophysical Journal Supplement Series | volume = 71 | pages = 245 | year = 1989 | bibcode = 1989ApJS...71..245K }}</ref>
* [[R Puppis]]<ref name="keenan">{{Cite journal | last1 = Keenan | first1 = P. C. | last2 = McNeil | first2 = R. C. | doi = 10.1086/191373 | title = The Perkins catalog of revised MK types for the cooler stars | journal = The Astrophysical Journal Supplement Series | volume = 71 | pages = 245 | year = 1989 | bibcode = 1989ApJS...71..245K }}</ref>
* [[IRC+10420]] (V1302 Aql)
* [[IRC+10420]] (V1302 Aql)
* [[IRAS 18357-0604]]
* [[IRAS 18357-0604]]<ref name=clark2014>{{Cite journal | doi = 10.1051/0004-6361/201322772| title = IRAS 18357-0604 – an analogue of the galactic yellow hypergiant IRC +10420?| journal = Astronomy & Astrophysics| volume = 561| pages = A15| year = 2013| last1 = Clark | first1 = J. S.| last2 = Negueruela | first2 = I.| last3 = González-Fernández | first3 = C.| bibcode = 2014A&A...561A..15C|arxiv = 1311.3956 | s2cid = 53372226}}</ref>
* [[V766 Centauri]] (= HR 5171A)<ref>{{Cite journal |last1=van Genderen |first1=A. M. |last2=Lobel |first2=A. |last3=Nieuwenhuijzen |first3=H. |last4=Henry |first4=G. W. |last5=de Jager |first5=C. |last6=Blown |first6=E. |last7=Di Scala |first7=G. |last8=van Ballegoij |first8=E. J. |date=November 2019 |title=Pulsations, eruptions, and evolution of four yellow hypergiants |url=https://www.aanda.org/10.1051/0004-6361/201834358 |journal=Astronomy & Astrophysics |volume=631 |pages=A48 |doi=10.1051/0004-6361/201834358 |arxiv=1910.02460 |bibcode=2019A&A...631A..48V |issn=0004-6361}}</ref>
* [[V766 Centauri]] (= HR 5171A) (possibly a red supergiant<ref name=wittkowski>{{cite journal|bibcode=2017A&A...597A...9W|arxiv=1610.01927|title=VLTI/AMBER spectro-interferometry of the late-type supergiants V766 Cen (=HR 5171 A), σ Oph, BM Sco, and HD 206859|journal=Astronomy & Astrophysics|volume=597|pages=A9|last1=Wittkowski|first1=M.|last2=Arroyo-Torres|first2=B.|last3=Marcaide|first3=J. M.|last4=Abellan|first4=F. J.|last5=Chiavassa|first5=A.|last6=Guirado|first6=J. C.|year=2017|doi=10.1051/0004-6361/201629349|s2cid=55679854}}</ref>)
* [[HD 179821]]
* [[HD 179821]]
* [[IRAS 17163-3907]]
* [[IRAS 17163-3907]]
* [[V382 Carinae]]
* [[V382 Carinae]]
* [[RSGC1-F15]]<ref name=davies>{{cite journal|doi=10.1086/527350|title=The Cool Supergiant Population of the Massive Young Star Cluster RSGC1|journal=The Astrophysical Journal|volume=676|issue=2|pages=1016–1028|year=2008|last1=Davies|first1=Ben|last2=Figer|first2=Don F.|last3=Law|first3=Casey J.|last4=Kudritzki|first4=Rolf‐Peter|last5=Najarro|first5=Francisco|last6=Herrero|first6=Artemio|last7=MacKenty|first7=John W.|bibcode=2008ApJ...676.1016D|arxiv = 0711.4757 |s2cid=15639297}}</ref>
* [[RSGC1-F15]]<ref name=davies>{{cite journal|doi=10.1086/527350|title=The Cool Supergiant Population of the Massive Young Star Cluster RSGC1|journal=The Astrophysical Journal|volume=676|issue=2|pages=1016–1028|year=2008|last1=Davies|first1=Ben|last2=Figer|first2=Don F.|last3=Law|first3=Casey J.|last4=Kudritzki|first4=Rolf-Peter|last5=Najarro|first5=Francisco|last6=Herrero|first6=Artemio|last7=MacKenty|first7=John W.|bibcode=2008ApJ...676.1016D|arxiv = 0711.4757 |s2cid=15639297}}</ref>
* [[V810 Centauri]]<ref>{{Cite journal |last=Garcia |first=B. |date=1989-06-01 |title=A list of MK standard stars |journal=Bulletin d'Information du Centre de Donnees Stellaires |volume=36 |pages=27 |bibcode=1989BICDS..36...27G |issn=1169-8837}}</ref>
*[[VdBH 222#371]]<ref>{{Cite journal|last1=Marco|first1=A.|last2=Negueruela|first2=I.|last3=González-Fernández|first3=C.|last4=Maíz Apellániz|first4=J.|last5=Dorda|first5=R.|last6=Clark|first6=J. S.|date=2014-07-01|title=VdBH 222: a starburst cluster in the inner Milky Way⋆|journal=Astronomy and Astrophysics|volume=567|pages=A73|doi=10.1051/0004-6361/201423897|arxiv=1405.7266|bibcode=2014A&A...567A..73M|s2cid=53533846|issn=0004-6361}}</ref>
*[[GLIMPSE20-1]]<ref>{{Cite journal |last1=Clark |first1=J. S. |last2=Ritchie |first2=B. W. |last3=Negueruela |first3=I. |date=2013-12-01 |title=The circumstellar environment and evolutionary state of the supergiant B[e] star Wd1-9 |journal=Astronomy and Astrophysics |volume=560 |pages=A11 |doi=10.1051/0004-6361/201321412 |arxiv=1311.4792 |bibcode=2013A&A...560A..11C |s2cid=53408838 |issn=0004-6361}}</ref><ref>{{Cite journal |last1=Messineo |first1=Maria |last2=Davies |first2=Ben |last3=Ivanov |first3=Valentin D. |last4=Figer |first4=Donald F. |last5=Schuller |first5=Frederic |last6=Habing |first6=Harm J. |last7=Menten |first7=Karl M. |last8=Petr-Gotzens |first8=Monika G. |date=2009-05-01 |title=Near-Infrared Spectra of Galactic Stellar Clusters Detected on Spitzer/GLIMPSE Images |journal=The Astrophysical Journal |volume=697 |issue=1 |pages=701–712 |doi=10.1088/0004-637X/697/1/701 |arxiv=0903.2238 |bibcode=2009ApJ...697..701M |s2cid=15823676 |issn=0004-637X}}</ref>
*[[2MASS J17444840-2902163]]<ref>{{Cite journal|last1=Clark|first1=J. S.|last2=Patrick|first2=L. R.|last3=Najarro|first3=F.|last4=Evans|first4=C. J.|last5=Lohr|first5=M.|date=2021-05-01|title=Constraining the population of isolated massive stars within the Central Molecular Zone|journal=Astronomy and Astrophysics|volume=649|pages=A43|doi=10.1051/0004-6361/202039205|arxiv=2102.08126|bibcode=2021A&A...649A..43C|s2cid=231934076|issn=0004-6361}}</ref>
*[[RW Cephei]]<ref>{{Cite journal |last1=Anugu |first1=Narsireddy |last2=Gies |first2=Douglas R. |last3=Roettenbacher |first3=Rachael M. |last4=Monnier |first4=John D. |last5=Montargés |first5=Miguel |last6=Mérand |first6=Antoine |last7=Baron |first7=Fabien |last8=Schaefer |first8=Gail H. |last9=Shepard |first9=Katherine A. |last10=Kraus |first10=Stefan |last11=Anderson |first11=Matthew D. |last12=Codron |first12=Isabelle |last13=Gardner |first13=Tyler |last14=Gutierrez |first14=Mayra |last15=Köhler |first15=Rainer |date=September 2024 |title=Time Evolution Images of the Hypergiant RW Cephei during the Rebrightening Phase Following the Great Dimming |journal=The Astrophysical Journal Letters |language=en |volume=973 |issue=1 |pages=L5 |doi=10.3847/2041-8213/ad736c |doi-access=free |arxiv=2408.11906 |bibcode=2024ApJ...973L...5A |issn=2041-8205}}</ref>
*[[Stephenson 2 DFK 49]]<ref>{{Cite journal |last1=Humphreys |first1=Roberta M. |last2=Helmel |first2=Greta |last3=Jones |first3=Terry J. |last4=Gordon |first4=Michael S. |date=2020-09-01 |title=Exploring the Mass-loss Histories of the Red Supergiants* |journal=The Astronomical Journal |volume=160 |issue=3 |pages=145 |doi=10.3847/1538-3881/abab15 |doi-access=free |arxiv=2008.01108 |bibcode=2020AJ....160..145H |issn=0004-6256}}</ref>


===In other galaxies===
In [[Westerlund 1]]:<ref name=clark>{{Cite journal | last1 = Clark | first1 = J. S. | last2 = Negueruela | first2 = I. | last3 = Crowther | first3 = P. A. | last4 = Goodwin | first4 = S. P. | title = On the massive stellar population of the super star cluster Westerlund 1 | doi = 10.1051/0004-6361:20042413 | journal = Astronomy and Astrophysics | volume = 434 | issue = 3 | pages = 949 | year = 2005 |arxiv = astro-ph/0504342 |bibcode = 2005A&A...434..949C }}</ref>
* [[HD 7583]] (R45 in SMC)<ref name=dejaeger>{{Cite journal | last1 = De Jager | first1 = C. | title = The yellow hypergiants | doi = 10.1007/s001590050009 | journal = Astronomy and Astrophysics Review | volume = 8 | issue = 3 | pages = 145–180 | year = 1998 |bibcode = 1998A&ARv...8..145D | s2cid = 189936279 }}</ref>
* W4
* W8a
* W12a
* W16a
* W32
* W265

In other galaxies:
* [[HD 7583]] (R45 in SMC)<ref name=dejaeger>{{Cite journal | last1 = De Jager | first1 = C. | title = The yellow hypergiants | doi = 10.1007/s001590050009 | journal = Astronomy and Astrophysics Review | volume = 8 | issue = 3 | pages = 145–180 | year = 1998 |bibcode = 1998A&ARv...8..145D }}</ref>
* [[HD 33579]] (in LMC)
* [[HD 33579]] (in LMC)
* [[HV 2450]] (in LMC, may be a red supergiant instead<ref>{{Cite journal |last1=Neugent |first1=Kathryn F. |last2=Massey |first2=Philip |last3=Skiff |first3=Brian |last4=Meynet |first4=Georges |date=2012-04-20 |title=Yellow and Red Supergiants in the Large Magellanic Cloud |url=https://iopscience.iop.org/article/10.1088/0004-637X/749/2/177 |journal=The Astrophysical Journal |volume=749 |issue=2 |pages=177 |doi=10.1088/0004-637X/749/2/177 |arxiv=1202.4225 |bibcode=2012ApJ...749..177N |issn=0004-637X}}</ref>)<ref name=":0">{{Cite journal |last1=Chen |first1=Kaitlyn M. |last2=Dorn-Wallenstein |first2=Trevor Z. |date=2024-03-01 |title=A Spectroscopic Hunt for Post-red Supergiants in the Large Magellanic Cloud. I. Preliminary Results |journal=Research Notes of the American Astronomical Society |volume=8 |issue=3 |pages=75 |arxiv=2403.08048 |bibcode=2024RNAAS...8...75C |doi=10.3847/2515-5172/ad32bb |issn=2515-5172 |doi-access=free}}</ref>
* [[HD 269723]] (R117 in LMC)<ref name="dejaeger"/>
* [[HD 269723]] (R117 in LMC)<ref name="dejaeger"/>
* [[HD 269953]] (R150 in LMC)<ref name="dejaeger"/>
* [[HD 269953]] (R150 in LMC)<ref name="dejaeger"/>
* [[HD 268757]] (R59 in LMC)<ref name="dejaeger"/>
* [[HD 268757]] (R59 in LMC)<ref name="dejaeger"/>
* [[SP77 31-16]] (in LMC)<ref name=":0" />
* Variable A (in [[Triangulum Galaxy|M33]])<ref name=humphreys>{{Cite journal | doi = 10.1088/0004-637X/790/1/48| title = LUMINOUS AND VARIABLE STARS IN M31 AND M33. II. LUMINOUS BLUE VARIABLES, CANDIDATE LBVs, Fe II EMISSION LINE STARS, AND OTHER SUPERGIANTS| journal = The Astrophysical Journal| volume = 790| issue = 1| pages = 48| year = 2014| last1 = Humphreys | first1 = R. M. | last2 = Weis | first2 = K. | last3 = Davidson | first3 = K. | last4 = Bomans | first4 = D. J.| last5 = Burggraf | first5 = B. | bibcode = 2014ApJ...790...48H|arxiv = 1407.2259 | s2cid = 119177378}}</ref>
* B324 (in [[Triangulum Galaxy|M33]])<ref name=humphreys/>
* [[Var A|Variable A]] (in [[Triangulum Galaxy|M33]])
* [[Mothra (star)]] (in LS1)<ref name=humphreys>{{Cite journal | doi = 10.1088/0004-637X/790/1/48| title = Luminous and Variable Stars in M31 and M33. II. Luminous Blue Variables, Candidate LBVs, Fe II Emission Line Stars, and Other Supergiants| journal = The Astrophysical Journal| volume = 790| issue = 1| pages = 48| year = 2014| last1 = Humphreys | first1 = R. M. | last2 = Weis | first2 = K. | last3 = Davidson | first3 = K. | last4 = Bomans | first4 = D. J.| last5 = Burggraf | first5 = B. | bibcode = 2014ApJ...790...48H|arxiv = 1407.2259 | s2cid = 119177378}}</ref>
*LGGS J013250.70+304510.6<ref>Maria R. Drout; Philip Massey; Georges Meynet (2012). "The yellow and red supergiants of M33". The Astrophysical Journal. 750 (2): 97. arXiv:1203.0247. doi:10.1088/0004-637X/750/2/97.</ref>
* [[B324]] (in [[Triangulum Galaxy|M33]])<ref name=humphreys/><ref name=":1">{{Cite journal |last1=Kourniotis |first1=M. |last2=Bonanos |first2=A. Z. |last3=Yuan |first3=W. |last4=Macri |first4=L. M. |last5=Garcia-Alvarez |first5=D. |last6=Lee |first6=C.-H. |date=2017-05-01 |title=Monitoring luminous yellow massive stars in M 33: new yellow hypergiant candidates |url=https://www.aanda.org/articles/aa/full_html/2017/05/aa29146-16/aa29146-16.html |journal=Astronomy & Astrophysics |language=en |volume=601 |pages=A76 |doi=10.1051/0004-6361/201629146 |arxiv=1612.06853 |bibcode=2017A&A...601A..76K |issn=0004-6361}}</ref>
*[[Sextans A]] 7<ref>Britavskiy, N. E.; Bonanos, A. Z.; Herrero, A.; Cerviño, M.; García-Álvarez, D.; Boyer, M. L.; Masseron, T.; Mehner, A.; McQuinn, K. B. W. (November 2019). "Physical parameters of red supergiants in dwarf irregular galaxies in the Local Group". Astronomy and Astrophysics. 631. arXiv:1909.13378. Bibcode:2019A&A...631A..95B. doi:10.1051/0004-6361/201935212.</ref>

* [[LGGS J013358.05+304539.9]] (in [[Triangulum Galaxy|M33]])<ref name=":1" />
* [[LGGS J013351.84+303827.4]] (in [[Triangulum Galaxy|M33]])<ref name=":1" />
* [[LGGS J013345.15+303620.1]] (in [[Triangulum Galaxy|M33]])<ref name=":1" />
* [[LGGS J013415.42+302816.4]] (in [[Triangulum Galaxy|M33]])<ref name=":1" />
* [[SP77 48-6]] (in LMC)<ref name=":0" />
* [[HD 271182]] (in LMC)<ref name=":3">{{Cite journal |last1=Kourniotis |first1=M |last2=Kraus |first2=M |last3=Maryeva |first3=O |last4=Borges Fernandes |first4=M |last5=Maravelias |first5=G |date=2022-02-12 |title=Revisiting the evolved hypergiants in the Magellanic Clouds |url=https://academic.oup.com/mnras/article/511/3/4360/6527576 |journal=Monthly Notices of the Royal Astronomical Society |volume=511 |issue=3 |pages=4360–4376 |doi=10.1093/mnras/stac386 |doi-access=free |issn=0035-8711|arxiv=2202.04667 }}</ref>
* [[HD 271192]] (in LMC)<ref name=":3" />
* [[HD 270086]] (in LMC)<ref name=":3" />
* [[WOH G64]] (in LMC)<ref name=Munoz-Sanchez2024>{{cite arxiv|display-authors=etal|author=Munoz-Sanchez, G.|date=28 November 2024|title=The dramatic transition of the extreme Red Supergiant WOH G64 to a Yellow Hypergiant|arxiv=2411.19329}}</ref>
* [[10182-pr-1]] (in NGC 2403)<ref name=":4">{{Cite journal |last1=Humphreys |first1=Roberta M. |last2=Stangl |first2=Sarah |last3=Gordon |first3=Michael S. |last4=Davidson |first4=Kris |last5=Grammer |first5=Skyler H. |date=2019-01-01 |title=Luminous and Variable Stars in NGC 2403 and M81* |journal=The Astronomical Journal |volume=157 |issue=1 |pages=22 |doi=10.3847/1538-3881/aaf1ac |doi-access=free |arxiv=1811.06559 |bibcode=2019AJ....157...22H |issn=0004-6256}}</ref>
* [[ZH 553]] (in NGC 2403)<ref name=":4" />
* [[ZH 912]] (in NGC 2403)<ref name=":4" />
* [[ZH 884]] (in NGC 2403)<ref name=":4" />
* [[10584-11-1]] (in Messier 81)<ref name=":4" />
* [[10584-8-1]] (in Messier 81)<ref name=":4" />
* [[10584-8-2]] (in Messier 81)<ref name=":4" />
* [[ZH 244]] (in Messier 81)<ref name=":4" />
* [[ZH 224]] (in Messier 81)<ref name=":4" />
* [[10584-13-2]] (in Messier 81)<ref name=":4" />
* [[ZH 1143]] (in Messier 81)<ref name=":4" />
* [[ZH 1406]] (in Messier 81)<ref name=":4" />
* [[10584-25-2]] (in Messier 81)<ref name=":4" />
* [[10584-13-3]] (in Messier 81)<ref name=":4" />


==References==
==References==
Line 82: Line 106:


[[Category:Hypergiants|+]]
[[Category:Hypergiants|+]]
[[Category:Star types]]
[[Category:Stellar phenomena]]
[[Category:Stellar phenomena]]
[[Category:Articles containing video clips]]
[[Category:Articles containing video clips]]

Latest revision as of 14:04, 2 December 2024

Intrinsic variable types in the Hertzsprung–Russell diagram showing the Yellow Hypergiants above (i.e. more luminous than) the Cepheid instability strip

A yellow hypergiant (YHG) is a massive star with an extended atmosphere, a spectral class from A to K, and, starting with an initial mass of about 20–60 solar masses, has lost as much as half that mass. They are amongst the most visually luminous stars, with absolute magnitude (MV) around −9, but also one of the rarest, with just 20 known in the Milky Way and six of those in just a single cluster. They are sometimes referred to as cool hypergiants in comparison with O- and B-type stars, and sometimes as warm hypergiants in comparison with red supergiants.

Classification

[edit]

The term "hypergiant" was used as early as 1929, but not for the stars currently known as hypergiants.[1] Hypergiants are defined by their '0' luminosity class, and are higher in luminosity than the brightest supergiants of class Ia,[2] although they were not referred to as hypergiants until the late 1970s.[3] Another criterion for hypergiants was also suggested in 1979 for some other highly luminous mass-losing hot stars,[4] but was not applied to cooler stars. In 1991, Rho Cassiopeiae was the first to be described as a yellow hypergiant,[5] likely becoming grouped as a new class of luminous stars during discussions at the Solar physics and astrophysics at interferometric resolution workshop in 1992.[6]

Definitions of the term hypergiant remain vague, and although luminosity class 0 is for hypergiants, they are more commonly designated by the alternative luminosity classes Ia-0 and Ia+.[7] Their great stellar luminosities are determined from various spectral features, which are sensitive to surface gravity, such as Hβ line widths in hot stars or a strong Balmer discontinuity in cooler stars. Lower surface gravity often indicates larger stars, and hence, higher luminosities.[8] In cooler stars, the strength of observed oxygen lines, such as O I at 777.4 nm., can be used to calibrate directly against stellar luminosity.[9]

One astrophysical method used to definitively identify yellow hypergiants is the so-called Keenan-Smolinski criterion. Here all absorption lines should be strongly broadened, beyond those expected of bright supergiant stars, and also show strong evidence of significant mass loss. Furthermore, at least one broadened component should also be present. They may also display very complex Hα profiles, typically having strong emission lines combined with absorption lines.[10]

The terminology of yellow hypergiants is further complicated by referring to them as either cool hypergiants or warm hypergiants, depending on the context. Cool hypergiants refers to all sufficiently luminous and unstable stars cooler than blue hypergiants and LBVs, including both yellow and red hypergiants.[11] The term warm hypergiants has been used for highly luminous class A and F stars in M31 and M33 that are not LBVs,[12] as well as more generally for yellow hypergiants.[13]

Characteristics

[edit]
Visual light curve for ρ Cassiopeiae from 1933 to 2015

Yellow hypergiants occupy a region of the Hertzsprung–Russell diagram above the instability strip, a region where relatively few stars are found and where those stars are generally unstable. The spectral and temperature ranges are approximately A0-K2 and 4,000–8,000 K (3,730–7,730 °C; 6,740–13,940 °F) respectively. The area is bounded on the high-temperature side by the Yellow Evolutionary Void where stars of this luminosity become extremely unstable and experience severe mass loss. The “Yellow Evolutionary Void” separates yellow hypergiants from luminous blue variables although yellow hypergiants at their hottest and luminous blue variables at their coolest can have approximately the same temperature near 8,000 K. At the lower temperature bound, yellow hypergiants and red supergiants are not clearly separated; RW Cephei (roughly 4,000 K (3,730 °C; 6,740 °F), 295,000 L) is an example of a star that shares characteristics of both yellow hypergiants and red supergiants.[14][15]

Yellow hypergiants have a fairly narrow range of luminosities above 200,000 L (e.g. V382 Carinae at 212,000 L) and below the Humphrey-Davidson limit at around 600,000 L. With their output peaking in the middle of the visual range, these are the most visually bright stars known with absolute magnitudes around −9 or −9.5 .[5]

They are large and somewhat unstable, with very low surface gravities. Where yellow supergiants have surface gravities (log g) below about 2, the yellow hypergiants have log g around zero. In addition they pulsate irregularly, producing small variations in temperature and brightness. This produces very high mass loss rates, and nebulosity is common around the stars.[16] Occasional larger outbursts can temporarily obscure the stars.[17]

Yellow hypergiants form from massive stars after they have evolved away from the main sequence. Most observed yellow hypergiants have been through a red supergiant phase and are evolving back towards higher temperatures, but a few are seen in the brief first transition from main sequence to red supergiant. Supergiants with an initial mass less than 20 M will explode as a supernova while still red supergiants, while stars more massive than about 60 M will never cool beyond blue supergiant temperatures. The exact mass ranges depend on metallicity and rotation.[18] Yellow supergiants cooling for the first time may be massive stars of up to 60 M or more,[15] but post-red supergiant stars will have lost around half their initial mass.[19]

Chemically, most yellow hypergiants show strong surface enhancement of nitrogen and also of sodium and some other heavy elements. Carbon and oxygen are depleted, while helium is enhanced, as expected for a post-main-sequence star.

Evolution

[edit]

Yellow hypergiants have clearly evolved off the main sequence and so have depleted the hydrogen in their cores. The majority of yellow hypergiants are postulated to be post-red supergiants evolving blueward,[14] while more stable and less luminous yellow supergiants are likely to be evolving to red supergiants for the first time. There is strong chemical and surface gravity evidence that the brightest of the yellow supergiants, HD 33579, is currently expanding from a blue supergiant to a red supergiant.[15]

These stars are doubly rare because they are very massive, initially hot class O-type main-sequence stars more than 15 times as massive as the Sun, but also because they spend only a few thousand years in the unstable yellow void phase of their lives. In fact, it is difficult to explain even the small number of observed yellow hypergiants, relative to red supergiants of comparable luminosity, from simple models of stellar evolution. The most luminous red supergiants may execute multiple "blue loops", shedding much of their atmosphere, but without actually ever reaching the blue supergiant stage, each one taking only a few decades at most. Conversely, some apparent yellow hypergiants may be hotter stars, such as the "missing" LBVs, masked within a cool pseudo-photosphere.[14]

Recent discoveries of blue supergiant supernova progenitors have also raised the question of whether stars could explode directly from the yellow hypergiant stage.[20] A handful of possible yellow supergiant supernova progenitors have been discovered, but they all appear to be of relatively low mass and luminosity, not hypergiants.[21][22] SN 2013cu is a type IIb supernova whose progenitor has been directly and clearly observed. It was an evolved star around 8,000 K (7,730 °C; 13,940 °F) showing extreme mass loss of helium and nitrogen enriched material. Although the luminosity is not known, only a yellow hypergiant or luminous blue variable in outburst would have these properties.[23]

Modern models suggest that stars with a certain range of masses and rotation rates may explode as supernovae without ever becoming blue supergiants again, but many will eventually pass right through the yellow void and become low-mass low-luminosity luminous blue variables and possibly Wolf–Rayet stars after that.[24] Specifically, more massive stars and those with higher mass loss rates due to rotation or high metallicity will evolve beyond the yellow hypergiant stage to hotter temperatures before reaching core collapse.[25]

Structure

[edit]
IRAS 17163-3907 is a yellow hypergiant that clearly shows the expelled material that probably surrounds all yellow hypergiants.

According to the current physical models of stars, a yellow hypergiant should possess a convective core surrounded by a radiative zone, as opposed to a sun-sized star, which consists of a radiative core surrounded by a convective zone.[26] Because of their extreme luminosity and internal structure,[27] yellow hypergiants suffer high rates of mass loss[28] and are generally surrounded by envelopes of expelled material. An example of the nebulae that can result is IRAS 17163-3907, known as the Fried Egg, which has expelled several solar masses of material in just a few hundred years.[29]

The yellow hypergiant is an expected phase of evolution as the most luminous red supergiants evolve bluewards, but they may also represent a different sort of star. LBVs during eruption have such dense winds that they form a pseudo-photosphere which appears as a larger cooler star despite the underlying blue supergiant being largely unchanged. These are observed to have a very narrow range of temperatures around 8,000 K (7,730 °C; 13,940 °F). At the bistability jump which occurs around 21,000 K (20,700 °C; 37,300 °F) blue supergiant winds become several times denser and could be result in an even cooler pseudo-photosphere. No LBVs are observed just below the luminosity where the bistability jump crosses the S Doradus instability strip (not to be confused with the Cepheid instability strip), but it is theorised that they do exist and appear as yellow hypergiants because of their pseudo-photospheres.[30]

Known yellow hypergiants

[edit]
Yellow hypergiant HR 5171 A, seen as the bright yellow star at the center of the image.
Artist's impression of the binary system containing yellow hypergiant HR 5171 A

In Milky Way galaxy

[edit]

In other galaxies

[edit]

References

[edit]
  1. ^ Wallenquist, Aå (1929). "An attempt to determine the mean masses of the stars in the globular cluster M 3". Bulletin of the Astronomical Institutes of the Netherlands. 5: 67. Bibcode:1929BAN.....5...67W.
  2. ^ Morgan, William Wilson; Keenan, Philip Childs; Kellman, Edith (1943). "An atlas of stellar spectra, with an outline of spectral classification". Chicago. Bibcode:1943assw.book.....M.
  3. ^ De Jager, Cornelis (1980). "The Main Observational Characteristics of the Most Luminous Stars". The Brightest Stars. pp. 18–56. doi:10.1007/978-94-009-9030-2_2. ISBN 978-90-277-1110-6.
  4. ^ Llorente De Andres, F.; Lamers, H. J. G. L. M.; Muller, E. A. (1979). "Line Blocking in the Near Ultraviolet Spectrum of Early-Type Stars—Part Two—the Dependence on Spectral Type and Luminosity for Normal Stars". Astronomy and Astrophysics Supplement. 38: 367. Bibcode:1979A&AS...38..367L.
  5. ^ a b Zsoldos, E.; Percy, J. R. (1991). "Photometry of yellow semiregular variables - Rho Cassiopeiae". Astronomy and Astrophysics. 246: 441. Bibcode:1991A&A...246..441Z. ISSN 0004-6361.
  6. ^ De Jager, Cornelis; Nieuwenhuijzen, Hans (1992). "Yellow hypergiant interferometry: A clue to understanding evolutionary instability". In ESA. 344: 109. Bibcode:1992ESASP.344..109D.
  7. ^ Achmad, L.; Lamers, H. J. G. L. M.; Nieuwenhuijzen, H.; Van Genderen, A. M. (1992). "A photometric study of the G0-4 Ia(+) hypergiant HD 96918 (V382 Carinae)". Astronomy and Astrophysics. 259: 600. Bibcode:1992A&A...259..600A. ISSN 0004-6361.
  8. ^ Napiwotzki, R.; Schoenberner, D.; Wenske, V. (1993). "On the determination of effective temperature and surface gravity of B, A, and F stars using Stromgren UVBY beta photometry". Astronomy and Astrophysics. 268: 653. Bibcode:1993A&A...268..653N. ISSN 0004-6361.
  9. ^ Arellano Ferro, A.; Giridhar, S.; Rojo Arellano, E. (2003). "A Revised Calibration of the MV-W(O I 7774) Relationship using Hipparcos Data: Its Application to Cepheids and Evolved Stars". Revista Mexicana de Astronomía y Astrofísica. 39: 3. arXiv:astro-ph/0210695. Bibcode:2003RMxAA..39....3A.
  10. ^ a b c d e De Jager, C. (1998). "The yellow hypergiants". Astronomy and Astrophysics Review. 8 (3): 145–180. Bibcode:1998A&ARv...8..145D. doi:10.1007/s001590050009. S2CID 189936279.
  11. ^ Lobel, A.; De Jager, K.; Nieuwenhuijzen, H. (2013). "Long-term Spectroscopic Monitoring of Cool Hypergiants HR 8752, IRC+10420, and 6 Cas near the Yellow Evolutionary Void". 370 Years of Astronomy in Utrecht. Proceedings of a Conference Held 2–5 April. 470: 167. Bibcode:2013ASPC..470..167L.
  12. ^ Humphreys, Roberta M.; Davidson, Kris; Grammer, Skyler; Kneeland, Nathan; Martin, John C.; Weis, Kerstin; Burggraf, Birgitta (2013). "Luminous and Variable Stars in M31 and M33. I. The Warm Hypergiants and Post-Red Supergiant Evolution". The Astrophysical Journal. 773 (1): 46. arXiv:1305.6051. Bibcode:2013ApJ...773...46H. doi:10.1088/0004-637X/773/1/46. S2CID 118413197.
  13. ^ Shenoy, Dinesh; Humphreys, Roberta M.; Jones, Terry J.; Marengo, Massimo; Gehrz, Robert D.; Helton, L. Andrew; Hoffmann, William F.; Skemer, Andrew J.; Hinz, Philip M. (2016). "Searching for Cool Dust in the Mid-to-far Infrared: The Mass-loss Histories of the Hypergiants μ Cep, VY CMa, IRC+10420, and ρ Cas". The Astronomical Journal. 151 (3): 51. arXiv:1512.01529. Bibcode:2016AJ....151...51S. doi:10.3847/0004-6256/151/3/51. S2CID 119281306.
  14. ^ a b c Stothers, R. B.; Chin, C. W. (2001). "Yellow Hypergiants as Dynamically Unstable Post–Red Supergiant Stars". The Astrophysical Journal. 560 (2): 934. Bibcode:2001ApJ...560..934S. doi:10.1086/322438. hdl:2060/20010083764.
  15. ^ a b c Nieuwenhuijzen, H; de Jager, C (2000). "Checking the yellow evolutionary void. Three evolutionary critical Hypergiants: HD 33579, HR 8752 & IRC +10420". Astronomy and Astrophysics. 353: 163–176. Bibcode:2000A&A...353..163N.
  16. ^ Lobel, A.; Israelian, G.; de Jager, C.; Musaev, F.; Parker, J. W.; Mavrogiorgou, A. (1998). "The spectral variability of the cool hypergiant rho Cassiopeiae". Astronomy and Astrophysics. 330: 659–675. Bibcode:1998A&A...330..659L.
  17. ^ Lobel; Stefanik; Torres; Davis; Ilyin; Rosenbush (2003). "Spectroscopy of the Millennium Outburst and Recent Variability of the Yellow Hypergiant Rho Cassiopeiae". Stars as Suns: Activity. 219: 903. arXiv:astro-ph/0312074. Bibcode:2004IAUS..219..903L.
  18. ^ Groh, Jose H.; Meynet, Georges; Georgy, Cyril; Ekström, Sylvia (2013). "Fundamental properties of core-collapse supernova and GRB progenitors: Predicting the look of massive stars before death". Astronomy & Astrophysics. 558: A131. arXiv:1308.4681. Bibcode:2013A&A...558A.131G. doi:10.1051/0004-6361/201321906. S2CID 84177572.
  19. ^ Gesicki, K. (1992). "A Modelling of Circumstellar BAII Lines for the Hypergiant Rho-Cassiopeiae". Astronomy and Astrophysics. 254: 280. Bibcode:1992A&A...254..280G.
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