Stellar population

Last updated
Artist's conception of the spiral structure of the Milky Way showing Baade's general population categories. The blue regions in the spiral arms are composed of the younger population I stars, while the yellow stars in the central bulge are the older population II stars. In reality, many population I stars are also found mixed in with the older population II stars. Artist's impression of the Milky Way (updated - annotated).jpg
Artist's conception of the spiral structure of the Milky Way showing Baade's general population categories. The blue regions in the spiral arms are composed of the younger population I stars, while the yellow stars in the central bulge are the older population II stars. In reality, many population I stars are also found mixed in with the older population II stars.

In 1944, Walter Baade categorized groups of stars within the Milky Way into stellar populations. In the abstract of the article by Baade, he recognizes that Jan Oort originally conceived this type of classification in 1926. [1]

Contents

Baade observed that bluer stars were strongly associated with the spiral arms, and yellow stars dominated near the central galactic bulge and within globular star clusters. [2] Two main divisions were defined as Population I star and population II, with another newer, hypothetical division called population III added in 1978.

Among the population types, significant differences were found with their individual observed stellar spectra. These were later shown to be very important and were possibly related to star formation, observed kinematics, [3] stellar age, and even galaxy evolution in both spiral and elliptical galaxies. These three simple population classes usefully divided stars by their chemical composition or metallicity. [4] [5] [3]

By definition, each population group shows the trend where lower metal content indicates higher age of stars. Hence, the first stars in the universe (very low metal content) were deemed population III, old stars (low metallicity) as population II, and recent stars (high metallicity) as population I. [6] The Sun is considered population I, a recent star with a relatively high 1.4% metallicity. Note that astrophysics nomenclature considers any element heavier than helium to be a "metal", including chemical non-metals such as oxygen. [7]

Stellar development

Observation of stellar spectra has revealed that stars older than the Sun have fewer heavy elements compared with the Sun. [3] This immediately suggests that metallicity has evolved through the generations of stars by the process of stellar nucleosynthesis.

Formation of the first stars

Under current cosmological models, all matter created in the Big Bang was mostly hydrogen (75%) and helium (25%), with only a very tiny fraction consisting of other light elements such as lithium and beryllium. [8] When the universe had cooled sufficiently, the first stars were born as population III stars, without any contaminating heavier metals. This is postulated to have affected their structure so that their stellar masses became hundreds of times more than that of the Sun. In turn, these massive stars also evolved very quickly, and their nucleosynthetic processes created the first 26 elements (up to iron in the periodic table). [9]

Many theoretical stellar models show that most high-mass population III stars rapidly exhausted their fuel and likely exploded in extremely energetic pair-instability supernovae. Those explosions would have thoroughly dispersed their material, ejecting metals into the interstellar medium (ISM), to be incorporated into the later generations of stars. Their destruction suggests that no galactic high-mass population III stars should be observable. [10] However, some population III stars might be seen in high-redshift galaxies whose light originated during the earlier history of the universe. [11] Scientists have found evidence of an extremely small ultra metal-poor star, slightly smaller than the Sun, found in a binary system of the spiral arms in the Milky Way. The discovery opens up the possibility of observing even older stars. [12]

Stars too massive to produce pair-instability supernovae would have likely collapsed into black holes through a process known as photodisintegration. Here some matter may have escaped during this process in the form of relativistic jets, and this could have distributed the first metals into the universe. [13] [14] [a]

Formation of the observed stars

The oldest stars observed thus far, [10] known as population II, have very low metallicities; [16] [6] as subsequent generations of stars were born, they became more metal-enriched, as the gaseous clouds from which they formed received the metal-rich dust manufactured by previous generations of stars from population III.

As those population II stars died, they returned metal-enriched material to the interstellar medium via planetary nebulae and supernovae, enriching further the nebulae, out of which the newer stars formed. These youngest stars, including the Sun, therefore have the highest metal content, and are known as population I stars.

Chemical classification by Walter Baade

Population I stars

Population I star Rigel with reflection nebula IC 2118 Treasures3.jpg
Population I star Rigel with reflection nebula IC 2118

Population I stars are young stars with the highest metallicity out of all three populations and are more commonly found in the spiral arms of the Milky Way galaxy. The Sun is considered as an intermediate population I star, while the sun-like μ Arae is much richer in metals. [17] (The term "metal rich star" is used to describe stars with a significantly higher metallicity than the Sun; higher than can be explained by measurement error.)

Population I stars usually have regular elliptical orbits of the Galactic Center, with a low relative velocity. It was earlier hypothesized that the high metallicity of population I stars makes them more likely to possess planetary systems than the other two populations, because planets, particularly terrestrial planets, are thought to be formed by the accretion of metals. [18] However, observations of the Kepler Space Telescope data have found smaller planets around stars with a range of metallicities, while only larger, potential gas giant planets are concentrated around stars with relatively higher metallicity – a finding that has implications for theories of gas-giant formation. [19] Between the intermediate population I and the population II stars comes the intermediate disc population.

Population II stars

The Milky Way. Population II stars are in the galactic bulge and globular clusters. Milky way profile.svg
The Milky Way. Population II stars are in the galactic bulge and globular clusters.
Artist's impression of a field of population III stars 100 million years after the Big Bang. Massive, Population III Star in the Early Universe.jpg
Artist’s impression of a field of population III stars 100 million years after the Big Bang.

Population II, or metal-poor, stars are those with relatively little of the elements heavier than helium. These objects were formed during an earlier time of the universe. Intermediate population II stars are common in the bulge near the centre of the Milky Way, whereas population II stars found in the galactic halo are older and thus more metal-deficient. Globular clusters also contain high numbers of population II stars. [20]

A characteristic of population II stars is that despite their lower overall metallicity, they often have a higher ratio of "alpha elements" (elements produced by the alpha process, like oxygen and neon) relative to iron (Fe) as compared with population I stars; current theory suggests that this is the result of type II supernovas being more important contributors to the interstellar medium at the time of their formation, whereas type Ia supernova metal-enrichment came at a later stage in the universe's development. [21]

Scientists have targeted these oldest stars in several different surveys, including the HK objective-prism survey of Timothy C. Beers et al. [22] and the Hamburg-ESO survey of Norbert Christlieb et al., [23] originally started for faint quasars. Thus far, they have uncovered and studied in detail about ten ultra-metal-poor (UMP) stars (such as Sneden's Star, Cayrel's Star, BD +17° 3248) and three of the oldest stars known to date: HE 0107-5240, HE 1327-2326 and HE 1523-0901. Caffau's star was identified as the most metal-poor star yet when it was found in 2012 using Sloan Digital Sky Survey data. However, in February 2014 the discovery of an even lower-metallicity star was announced, SMSS J031300.36-670839.3 located with the aid of SkyMapper astronomical survey data. Less extreme in their metal deficiency, but nearer and brighter and hence longer known, are HD 122563 (a red giant) and HD 140283 (a subgiant).

Population III stars

Possible glow of population III stars imaged by NASA's Spitzer Space Telescope Ssc2005-22a1.jpg
Possible glow of population III stars imaged by NASA's Spitzer Space Telescope

Population III stars [24] are a hypothetical population of extremely massive, luminous and hot stars with virtually no "metals", except possibly for intermixing ejecta from other nearby, early population III supernovae. The term was first introduced by Neville J. Woolf in 1965. [25] [26] Such stars are likely to have existed in the very early universe (i.e., at high redshift) and may have started the production of chemical elements heavier than hydrogen, which are needed for the later formation of planets and life as we know it. [27] [28]

The existence of population III stars is inferred from physical cosmology, but they have not yet been observed directly. Indirect evidence for their existence has been found in a gravitationally lensed galaxy in a very distant part of the universe. [29] Their existence may account for the fact that heavy elements – which could not have been created in the Big Bang – are observed in quasar emission spectra. [9] They are also thought to be components of faint blue galaxies. These stars likely triggered the universe's period of reionization, a major phase transition of the hydrogen gas composing most of the interstellar medium. Observations of the galaxy UDFy-38135539 suggest that it may have played a role in this reionization process. The European Southern Observatory discovered a bright pocket of early population stars in the very bright galaxy Cosmos Redshift 7 from the reionization period around 800 million years after the Big Bang, at z = 6.60. The rest of the galaxy has some later redder population II stars. [27] [30] Some theories hold that there were two generations of population III stars. [31]

Artist's impression of the first stars, 400 million years after the Big Bang NASA-WMAP-first-stars.jpg
Artist's impression of the first stars, 400 million years after the Big Bang

Current theory is divided on whether the first stars were very massive or not. One possibility is that these stars were much larger than current stars: several hundred solar masses, and possibly up to 1,000 solar masses. Such stars would be very short-lived and last only 2–5 million years. [32] Such large stars may have been possible due to the lack of heavy elements and a much warmer interstellar medium from the Big Bang.[ citation needed ] Conversely, theories proposed in 2009 and 2011 suggest that the first star groups might have consisted of a massive star surrounded by several smaller stars. [33] [34] [35] The smaller stars, if they remained in the birth cluster, would accumulate more gas and could not survive to the present day, but a 2017 study concluded that if a star of 0.8 solar masses (M) or less was ejected from its birth cluster before it accumulated more mass, it could survive to the present day, possibly even in our Milky Way galaxy. [36]

Analysis of data of extremely low-metallicity population II stars such as HE 0107-5240, which are thought to contain the metals produced by population III stars, suggest that these metal-free stars had masses of 20~130 solar masses. [37] On the other hand, analysis of globular clusters associated with elliptical galaxies suggests pair-instability supernovae, which are typically associated with very massive stars, were responsible for their metallic composition. [38] This also explains why there have been no low-mass stars with zero metallicity observed, despite models constructed for smaller population III stars. [39] [40] Clusters containing zero-metallicity red dwarfs or brown dwarfs (possibly created by pair-instability supernovae [16] ) have been proposed as dark matter candidates, [41] [42] but searches for these types of MACHOs through gravitational microlensing have produced negative results.[ citation needed ]

Population III stars are considered seeds of black holes in the early universe. Unlike high-mass black hole seeds, such as direct collapse black holes, they would have produced light ones. If they could have grown to larger than expected masses, then they could have been quasi-stars, other hypothetical seeds of heavy black holes which would have existed in the early development of the Universe before hydrogen and helium were contaminated by heavier elements.

Detection of population III stars is a goal of NASA's James Webb Space Telescope. [43]

On 8 December 2022, astronomers reported the possible detection of Population III stars, in a high-redshift galaxy called RX J2129–z8He II. [44] [45]

See also

Notes

  1. It has been proposed that recent supernovae SN 2006gy and SN 2007bi may have been pair-instability supernovae where such super-massive population III stars exploded. Clark (2010) speculates that these stars could have formed relatively recently in dwarf galaxies, since they contain mainly primordial, metal-free interstellar matter. Past supernovae in these small galaxies could have ejected their metal-rich contents at speeds high enough for them to escape the galaxy, keeping the small galaxies' metal content very low. [15]

Related Research Articles

<span class="mw-page-title-main">Globular cluster</span> Spherical collection of stars

A globular cluster is a spheroidal conglomeration of stars that is bound together by gravity, with a higher concentration of stars towards its center. It can contain anywhere from tens of thousands to many millions of member stars, all orbiting in a stable, compact formation. Globular clusters are similar in form to dwarf spheroidal galaxies, and though globular clusters were long held to be the more luminous of the two, discoveries of outliers had made the distinction between the two less clear by the early 21st century. Their name is derived from Latin globulus. Globular clusters are occasionally known simply as "globulars".

<span class="mw-page-title-main">Supernova</span> Astrophysical phenomenon

A supernova is a powerful and luminous explosion of a star. A supernova occurs during the last evolutionary stages of a massive star, or when a white dwarf is triggered into runaway nuclear fusion. The original object, called the progenitor, either collapses to a neutron star or black hole, or is completely destroyed to form a diffuse nebula. The peak optical luminosity of a supernova can be comparable to that of an entire galaxy before fading over several weeks or months.

<span class="mw-page-title-main">Star formation</span> Process by which dense regions of molecular clouds in interstellar space collapse to form stars

Star formation is the process by which dense regions within molecular clouds in interstellar space, sometimes referred to as "stellar nurseries" or "star-forming regions", collapse and form stars. As a branch of astronomy, star formation includes the study of the interstellar medium (ISM) and giant molecular clouds (GMC) as precursors to the star formation process, and the study of protostars and young stellar objects as its immediate products. It is closely related to planet formation, another branch of astronomy. Star formation theory, as well as accounting for the formation of a single star, must also account for the statistics of binary stars and the initial mass function. Most stars do not form in isolation but as part of a group of stars referred as star clusters or stellar associations.

<span class="mw-page-title-main">HE 0107-5240</span> Extremely metal poor star in the constellation Phoenix

HE0107-5240 is an extremely metal-poor Population II star, located roughly 36000 light-years away from Earth. It is one of the most metal-poor stars known in our Galaxy, with a metallicity [Fe/H] = −5.2±0.2; i.e. it has just 1/160000 of the metal that the Sun has. Because of its very low metallicity, it is believed to be one of the earliest Population II stars to have formed. If so, then it is also very old, with an age of roughly 13 billion years. Because the star is not completely metal-free, it does not belong to the first generation of stars. These stars converted the pristine hydrogen, helium, and lithium formed by the Big Bang into heavier elements, such as carbon, oxygen, and metals.

<span class="mw-page-title-main">Cepheid variable</span> Type of variable star that pulsates radially

A Cepheid variable is a type of variable star that pulsates radially, varying in both diameter and temperature. It changes in brightness, with a well-defined stable period and amplitude. Cepheids are important cosmic benchmarks for scaling galactic and extragalactic distances; a strong direct relationship exists between a Cepheid variable's luminosity and its pulsation period.

<span class="mw-page-title-main">Superluminous supernova</span> Supernova at least ten times more luminous than a standard supernova

A super-luminous supernova is a type of stellar explosion with a luminosity 10 or more times higher than that of standard supernovae. Like supernovae, SLSNe seem to be produced by several mechanisms, which is readily revealed by their light-curves and spectra. There are multiple models for what conditions may produce an SLSN, including core collapse in particularly massive stars, millisecond magnetars, interaction with circumstellar material, or pair-instability supernovae.

<span class="mw-page-title-main">Wolf–Rayet star</span> Heterogeneous class of stars with unusual spectra

Wolf–Rayet stars, often abbreviated as WR stars, are a rare heterogeneous set of stars with unusual spectra showing prominent broad emission lines of ionised helium and highly ionised nitrogen or carbon. The spectra indicate very high surface enhancement of heavy elements, depletion of hydrogen, and strong stellar winds. The surface temperatures of known Wolf–Rayet stars range from 20,000 K to around 210,000 K, hotter than almost all other kinds of stars. They were previously called W-type stars referring to their spectral classification.

<span class="mw-page-title-main">Blue supergiant</span> Hot, luminous star with a spectral type of A9 or earlier

A blue supergiant (BSG) is a hot, luminous star, often referred to as an OB supergiant. They are usually considered to be those with luminosity class I and spectral class B9 or earlier, although sometimes A-class supergiants are also deemed blue supergiants.

<span class="mw-page-title-main">Messier 61</span> Galaxy in the constellation Virgo

Messier 61 is an intermediate barred spiral galaxy in the Virgo Cluster of galaxies. It was first discovered by Barnaba Oriani on May 5, 1779, six days before Charles Messier discovered the same galaxy. Messier had observed it on the same night as Oriani but had mistaken it for a comet. Its distance has been estimated to be 45.61 million light years from the Milky Way Galaxy. It is a member of the M61 Group of galaxies, which is a member of the Virgo II Groups, a series of galaxies and galaxy clusters strung out from the southern edge of the Virgo Supercluster.

<span class="mw-page-title-main">Metallicity</span> Relative abundance of heavy elements in a star or other astronomical object

In astronomy, metallicity is the abundance of elements present in an object that are heavier than hydrogen and helium. Most of the normal currently detectable matter in the universe is either hydrogen or helium, and astronomers use the word "metals" as convenient shorthand for "all elements except hydrogen and helium". This word-use is distinct from the conventional chemical or physical definition of a metal as an electrically conducting solid. Stars and nebulae with relatively high abundances of heavier elements are called "metal-rich" when discussing metallicity, even though many of those elements are called nonmetals in chemistry.

<span class="mw-page-title-main">IC 1613</span> Irregular dwarf galaxy in the constellation Cetus

IC 1613 is an irregular dwarf galaxy, visible in the constellation Cetus near the star 26 Ceti. It was discovered in 1906 by Max Wolf, and is approaching Earth at 234 km/s.

<span class="mw-page-title-main">Red clump</span> Clustering of stars in astronomy diagram

The red clump is a clustering of red giants in the Hertzsprung–Russell diagram at around 5,000 K and absolute magnitude (MV) +0.5, slightly hotter than most red-giant-branch stars of the same luminosity. It is visible as a denser region of the red-giant branch or a bulge towards hotter temperatures. It is prominent in many galactic open clusters, and it is also noticeable in many intermediate-age globular clusters and in nearby field stars.

<span class="mw-page-title-main">Initial mass function</span> Empirical function in astronomy

In astronomy, the initial mass function (IMF) is an empirical function that describes the initial distribution of masses for a population of stars during star formation. IMF not only describes the formation and evolution of individual stars, it also serves as an important link that describes the formation and evolution of galaxies.

<span class="mw-page-title-main">Stellar kinematics</span> Study of the movement of stars

In astronomy, stellar kinematics is the observational study or measurement of the kinematics or motions of stars through space.

Canes Venatici II or CVn II is a dwarf spheroidal galaxy situated in the Canes Venatici constellation and discovered in 2006 in data obtained by the Sloan Digital Sky Survey. The galaxy is located at a distance of about 150 kpc from the Sun and moves towards the Sun with the velocity of about 130 km/s. It is classified as a dwarf spheroidal galaxy (dSph) meaning that it has an elliptical shape with a half-light radius of about 74+14
−10
 pc
.

The metallicity distribution function is an important concept in stellar and galactic evolution. It is a curve of what proportion of stars have a particular metallicity of a population of stars such as in a cluster or galaxy.

<span class="mw-page-title-main">Galactic habitable zone</span> Region of a galaxy in which life might most likely develop

In astrobiology and planetary astrophysics, the galactic habitable zone is the region of a galaxy in which life is most likely to develop. The concept of a galactic habitable zone analyzes various factors, such as metallicity and the rate and density of major catastrophes such as supernovae, and uses these to calculate which regions of a galaxy are more likely to form terrestrial planets, initially develop simple life, and provide a suitable environment for this life to evolve and advance. According to research published in August 2015, very large galaxies may favor the birth and development of habitable planets more than smaller galaxies such as the Milky Way. In the case of the Milky Way, its galactic habitable zone is commonly believed to be an annulus with an outer radius of about 10 kiloparsecs (33,000 ly) and an inner radius close to the Galactic Center.

A stellar halo is the component of a galaxy's galactic halo that contains stars. The stellar halo extends far outside a galaxy's brightest regions and typically contains its oldest and most metal poor stars.

<span class="mw-page-title-main">Hypernova</span> Supernova that ejects a large mass at unusually high velocity

A hypernova is a very energetic supernova which is believed to result from an extreme core collapse scenario. In this case, a massive star collapses to form a rotating black hole emitting twin astrophysical jets and surrounded by an accretion disk. It is a type of stellar explosion that ejects material with an unusually high kinetic energy, an order of magnitude higher than most supernovae, with a luminosity at least 10 times greater. Hypernovae release such intense gamma rays that they often appear similar to a type Ic supernova, but with unusually broad spectral lines indicating an extremely high expansion velocity. Hypernovae are one of the mechanisms for producing long gamma ray bursts (GRBs), which range from 2 seconds to over a minute in duration. They have also been referred to as superluminous supernovae, though that classification also includes other types of extremely luminous stellar explosions that have different origins.

<span class="mw-page-title-main">GCIRS 16SW</span> Binary star in the Galactic Center in the constellation Sagittarius

GCIRS 16SW, also known as S97, is a contact binary star located in the Galactic Center. It is composed of two hot massive stars of equal size that orbit each other with a period of 19.5 days. The stars are so close that their atmospheres overlap, and the two stars form an eclipsing binary varying in brightness by 0.35 magnitudes at infrared wavelengths.

References

  1. Baade, W. (1944). "The resolution of Messier 32, NGC 205, and the central region of the Andromeda nebula". Astrophysical Journal. 100: 137–146. Bibcode:1944ApJ...100..137B. doi: 10.1086/144650 . The two types of stellar populations had been recognized among the stars of our own galaxy by Oort as early as 1926.
  2. Shapley, Harlow (1977). Hodge, Paul (ed.). Galaxies (3 ed.). Harvard University Press. pp.  62–63. ISBN   978-0674340510 via Archive.org.
  3. 1 2 3 Gibson, B.K.; Fenner, Y.; Renda, A.; Kawata, D.; Hyun-chul, L. (2013). "Review: Galactic chemical evolution" (PDF). Publications of the Astronomical Society of Australia. 20 (4). CSIRO publishing: 401–415. arXiv: astro-ph/0312255 . Bibcode:2003PASA...20..401G. doi:10.1071/AS03052. S2CID   12253299. Archived from the original (PDF) on 20 January 2021. Retrieved 17 April 2018.
  4. Kunth, Daniel & Östlin, Göran (2000). "The most metal-poor galaxies". The Astronomy and Astrophysics Review . 10 (1): 1–79. arXiv: astro-ph/9911094 . Bibcode:2000A&ARv..10....1K. doi:10.1007/s001590000005. S2CID   15487742 . Retrieved 3 January 2022 via caltech.edu.
  5. Schönrich, R.; Binney, J. (2009). "Origin and structure of the Galactic disc(s)". Monthly Notices of the Royal Astronomical Society. 399 (3): 1145–1156. arXiv: 0907.1899 . Bibcode:2009MNRAS.399.1145S. doi: 10.1111/j.1365-2966.2009.15365.x .
  6. 1 2 Bryant, Lauren J. "What makes stars tick". Research & Creative Activity. Indiana University. Archived from the original on May 16, 2016. Retrieved September 7, 2005.
  7. "Metals". astronomy.swin.edu.au. Cosmos. Retrieved 2022-04-01.
  8. Cyburt, Richard H.; Fields, Brian D.; Olive, Keith A.; Yeh, Tsung-Han (2016). "Big bang nucleosynthesis: Present status". Reviews of Modern Physics . 88 (1): 015004. arXiv: 1505.01076 . Bibcode:2016RvMP...88a5004C. doi:10.1103/RevModPhys.88.015004. S2CID   118409603.
  9. 1 2 Heger, A.; Woosley, S.E. (2002). "The nucleosynthetic signature of Population III". Astrophysical Journal . 567 (1): 532–543. arXiv: astro-ph/0107037 . Bibcode:2002ApJ...567..532H. doi:10.1086/338487. S2CID   16050642.
  10. 1 2 Schlaufman, Kevin C.; Thompson, Ian B.; Casey, Andrew R. (2018). "An ultra metal-poor star near the hydrogen-burning Limit". The Astrophysical Journal. 867 (2): 98. arXiv: 1811.00549 . Bibcode:2018ApJ...867...98S. doi: 10.3847/1538-4357/aadd97 . S2CID   54511945.
  11. Xu, Hao; Wise, John H.; Norman, Michael L. (29 July 2013). "Population III stars and remnants in high-redshift galaxies". The American Astronomical Society. 773 (2): 83. arXiv: 1305.1325 . Bibcode:2013ApJ...773...83X. doi:10.1088/0004-637X/773/2/83. S2CID   118303030.
  12. "One of Milky Way's oldest stars discovered". Sci-News. 6 November 2018. Retrieved 12 June 2020.
  13. Fryer, C. L.; Woosley, S. E.; Heger, A. (2001). "Pair-instability supernovae, gravity waves, and gamma-ray transients". The Astrophysical Journal. 550 (1): 372–382. arXiv: astro-ph/0007176 . Bibcode:2001ApJ...550..372F. doi:10.1086/319719. S2CID   7368009.
  14. Heger, A.; Fryer, C. L.; Woosley, S. E.; Langer, N.; Hartmann, D. H. (2003). "How massive single stars end their life". The Astrophysical Journal. 591 (1): 288–300. arXiv: astro-ph/0212469 . Bibcode:2003ApJ...591..288H. doi:10.1086/375341. S2CID   59065632.
  15. Clark, Stuart (February 2010). "Primordial giant: The star that time forgot". New Scientist . Retrieved 1 February 2015.
  16. 1 2 Salvaterra, R.; Ferrara, A.; Schneider, R. (2004). "Induced formation of primordial low-mass stars". New Astronomy. 10 (2): 113–120. arXiv: astro-ph/0304074 . Bibcode:2004NewA...10..113S. doi:10.1016/j.newast.2004.06.003. S2CID   15085880.
  17. Soriano, M.S.; Vauclair, S. (2009). "New seismic analysis of the exoplanet-host star Mu Arae". Astronomy and Astrophysics. 513: A49. arXiv: 0903.5475 . Bibcode:2010A&A...513A..49S. doi:10.1051/0004-6361/200911862. S2CID   5688996.
  18. Lineweaver, Charles H. (2000). "An estimate of the age distribution of terrestrial planets in the universe: Quantifying metallicity as a selection effect". Icarus. 151 (2): 307–313. arXiv: astro-ph/0012399 . Bibcode:2001Icar..151..307L. doi:10.1006/icar.2001.6607. S2CID   14077895.
  19. Buchhave, L.A.; et al. (2012). "An abundance of small exoplanets around stars with a wide range of metallicities". Nature . 486 (7403): 375–377. Bibcode:2012Natur.486..375B. doi:10.1038/nature11121. PMID   22722196. S2CID   4427321.
  20. van Albada, T. S.; Baker, N. (1973). "On the two Oosterhoff groups of globular clusters". Astrophysical Journal . 185: 477–498. Bibcode:1973ApJ...185..477V. doi: 10.1086/152434 .
  21. Wolfe, Arthur M.; Gawiser, Eric; Prochaska, Jason X. (2005). "Damped Ly‑α systems". Annual Review of Astronomy and Astrophysics. 43 (1): 861–918. arXiv: astro-ph/0509481 . Bibcode:2005ARA&A..43..861W. doi:10.1146/annurev.astro.42.053102.133950. S2CID   119368187.
  22. Beers, T. C.; Preston, G. W.; Shectman, S. A. (1992). "A Search for Stars of Very Low Metal Abundance. II". Astronomical Journal . 103: 1987. Bibcode:1992AJ....103.1987B. doi:10.1086/116207. S2CID   121564385.
  23. Christlieb, N.; Wisotzki, L.; Reimers, D.; Gehren, T.; Reetz, J.; Beers, T. C. (1998). "An Automated Search for Metal-Poor Halo Stars in the Hamburg/ESO Objective-Prism Survey". ASP Conference Series. 666. arXiv: astro-ph/9810183v1 .
  24. Tominga, N.; et al. (2007). "Supernova nucleosynthesis in population III 13-50 Msolar stars and abundance patterns of extremely metal-poor stars". Astrophysical Journal . 660 (5): 516–540. arXiv: astro-ph/0701381 . Bibcode:2007ApJ...660..516T. doi:10.1086/513063. S2CID   119496577.
  25. Green, Louis (April 1966). "Observational Aspects of Cosmology". Sky and Telescope. 31: 199. Bibcode:1966S&T....31..199G.
  26. Thornton, Page (March 1966). "Observational Aspects of Cosmology". Science. 151 (3716): 1411–1414, 1416–1418. Bibcode:1966Sci...151.1411P. doi:10.1126/science.151.3716.1411. PMID   17817304.
  27. 1 2 Sobral, David; Matthee, Jorryt; Darvish, Behnam; Schaerer, Daniel; Mobasher, Bahram; Röttgering, Huub J.A.; Santos, Sérgio; Hemmati, Shoubaneh (4 June 2015). "Evidence for Pop III-like stellar populations in the most luminous Lyman-α emitters at the epoch of re-ionisation: Spectroscopic confirmation". The Astrophysical Journal . 808 (2): 139. arXiv: 1504.01734 . Bibcode:2015ApJ...808..139S. doi:10.1088/0004-637x/808/2/139. S2CID   18471887.
  28. Overbye, Dennis (17 June 2015). "Astronomers report finding earliest stars that enriched the cosmos". The New York Times . Retrieved 17 June 2015.
  29. Fosbury, R.A.E.; et al. (2003). "Massive star formation in a gravitationally lensed H II galaxy at z = 3.357". Astrophysical Journal . 596 (1): 797–809. arXiv: astro-ph/0307162 . Bibcode:2003ApJ...596..797F. doi:10.1086/378228. S2CID   17808828.
  30. "Best observational evidence of first-generation stars in the universe". Astronomy Magazine . 17 June 2015.
  31. Bromm, V.; Yoshida, N.; Hernquist, L.; McKee, C.F. (2009). "The formation of the first stars and galaxies". Nature . 459 (7243): 49–54. arXiv: 0905.0929 . Bibcode:2009Natur.459...49B. doi:10.1038/nature07990. PMID   19424148. S2CID   10258026.
  32. Ohkubo, Takuya; Nomoto, Ken'ichi; Umeda, Hideyuki; Yoshida, Naoki; Tsuruta, Sachiko (2009-12-01). "Evolution of very massive Population III stars with mass accretion from pre-main sequence to collapse". The Astrophysical Journal . 706 (2): 1184–1193. arXiv: 0902.4573 . Bibcode:2009ApJ...706.1184O. doi: 10.1088/0004-637X/706/2/1184 . ISSN   0004-637X.
  33. Redd, Nola (February 2011). "The universe's first stars weren't loners after all". Space.com. Retrieved 1 February 2015.
  34. Thompson, Andrea (January 2009). "How massive stars form: Simple solution found". Space.com. Retrieved 1 February 2015.
  35. Carr, Bernard J. "Cosmology, Population III". California Institute of Technology.
  36. Dutta, J.; Sur, S.; Stacy, A.; Bagla, J.S. (2020). "Modeling the Survival of Population III Stars to the Present Day". The Astrophysical Journal. 901 (1): 16. arXiv: 1712.06912 . Bibcode:2020ApJ...901...16D. doi: 10.3847/1538-4357/abadf8 . S2CID   209386374.
  37. Umeda, Hideyuki; Nomoto, Ken'Ichi (2003). "First-generation black-hole-forming supernovae and the metal abundance pattern of a very iron-poor star". Nature . 422 (6934): 871–873. arXiv: astro-ph/0301315 . Bibcode:2003Natur.422..871U. doi:10.1038/nature01571. PMID   12712199. S2CID   4424736.
  38. Puzia, Thomas H.; Kissler-Patig, Markus; Goudfrooij, Paul (2006). "Extremely α-enriched globular clusters in early-type galaxies: A step toward the dawn of stellar populations?". The Astrophysical Journal . 648 (1): 383–388. arXiv: astro-ph/0605210 . Bibcode:2006ApJ...648..383P. doi:10.1086/505679. S2CID   9815509.
  39. Siess, Lionel; Livio, Mario; Lattanzio, John (2002). "Structure, evolution, and nucleosynthesis of primordial stars". The Astrophysical Journal . 570 (1): 329–343. arXiv: astro-ph/0201284 . Bibcode:2002ApJ...570..329S. doi:10.1086/339733. S2CID   18385975.
  40. Gibson, Carl H.; Nieuwenhuizen, Theo M.; Schild, Rudolph E. (2013). "Why are so many primitive stars observed in the Galaxy halo". Journal of Cosmology. 22: 10163. arXiv: 1206.0187 . Bibcode:2013JCos...2210163G.
  41. Kerins, E.J. (1997). "Zero-metallicity very low mass stars as halo dark matter". Astronomy and Astrophysics . 322: 709. arXiv: astro-ph/9610070 . Bibcode:1997A&A...322..709K.
  42. Sanchez-Salcedo, F.J. (1997). "On the stringent constraint on massive dark clusters in the galactic halo". Astrophysical Journal Letters. 487 (1): L61. Bibcode:1997ApJ...487L..61S. doi: 10.1086/310873 .
  43. Rydberg, C.-E.; Zackrisson, E.; Lundqvist, P.; Scott, P. (March 2013). "Detection of isolated population III stars with the James Webb Space Telescope". Monthly Notices of the Royal Astronomical Society . 429 (4): 3658–3664. arXiv: 1206.0007 . Bibcode:2013MNRAS.429.3658R. doi: 10.1093/mnras/sts653 .
  44. Wang, Xin; et al. (8 December 2022). "A strong He II λ1640 emitter with extremely blue UV spectral slope at z=8.16: presence of Pop III stars?". arXiv: 2212.04476 [astro-ph.GA].
  45. Callaghan, Jonathan (30 January 2023). "Astronomers Say They Have Spotted the Universe's First Stars - Theory has it that "Population III" stars brought light to the cosmos. The James Webb Space Telescope may have just glimpsed them". Quanta Magazine . Retrieved 31 January 2023.

Further reading