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{{short description|Compact exotic star which forms matter consisting mostly of quarks}}
{{short description|Compact exotic star which forms matter consisting mostly of quarks}}
{{confused|Quasar}}
{{distinguish|Quasar|Q star}}
{{more citations needed|date=December 2015}}
{{More citations needed|date=March 2024}}
A '''quark star''' is a hypothetical type of [[compact star|compact]], [[exotic star]], where extremely high core temperature and pressure has forced [[Nucleon|nuclear particles]] to form [[quark matter]], a continuous [[state of matter]] consisting of free [[quark]]s.
A '''quark star''' is a hypothetical type of [[compact star|compact]], [[exotic star]], where extremely high core temperature and pressure have forced [[Nucleon|nuclear particles]] to form [[quark matter]], a continuous [[state of matter]] consisting of free [[quark]]s.<ref>{{cite news |last1=Sutter |first1=Paul |title=These Stars Are Like Nothing Else You’ll Ever See |url=https://www.popularmechanics.com/space/deep-space/a45456628/cosmologist-explains-weird-quark-stars/ |access-date=6 July 2024 |publisher=Popular Mechanics |date=5 October 2023}}</ref>


==Background==
==Background==
{{Unreferenced section|date=March 2024}}
Some [[star#Massive stars|massive stars]] collapse to form [[neutron stars]] at the end of their [[stellar life cycle|life cycle]], as has been both observed and explained theoretically. Under the extreme temperatures and pressures inside neutron stars, the neutrons are normally kept apart by a [[degeneracy pressure]], stabilizing the star and hindering further gravitational collapse. However, it is hypothesized that under even more extreme temperature and pressure, the degeneracy pressure of the neutrons is overcome, and the [[neutrons]] are forced to merge and dissolve into their constituent quarks, creating an ultra-dense [[Phase (matter)|phase]] of [[quark matter]] based on densely packed quarks. In this state, a new equilibrium is supposed to emerge, as a new degeneracy pressure between the quarks, as well as repulsive [[electromagnetic force]]s, will occur and hinder [[black hole|total gravitational collapse]].
Some [[star#Massive stars|massive stars]] collapse to form [[neutron stars]] at the end of their [[stellar life cycle|life cycle]], as has been both observed and explained theoretically. Under the extreme temperatures and pressures inside neutron stars, the neutrons are normally kept apart by a [[degeneracy pressure]], stabilizing the star and hindering further gravitational collapse.<ref>{{Cite web |last=Seife |first=Charles |title=Quark Stars Get Real |url=https://www.science.org/content/article/quark-stars-get-real |website=Science.org}}</ref> However, it is hypothesized that under even more extreme temperature and pressure, the degeneracy pressure of the neutrons is overcome, and the [[neutrons]] are forced to merge and dissolve into their constituent quarks, creating an ultra-dense [[Phase (matter)|phase]] of [[quark matter]] based on densely packed quarks. In this state, a new equilibrium is supposed to emerge, as a new degeneracy pressure between the quarks, as well as repulsive [[electromagnetic force]]s, will occur and hinder [[black hole|total gravitational collapse]].


If these ideas are correct, quark stars might occur, and be observable, somewhere in the universe. Theoretically, such a scenario is seen as scientifically plausible, but it has been impossible to prove both observationally and experimentally, because the very extreme conditions needed for stabilizing quark matter cannot be created in any laboratory nor observed directly in nature. The stability of quark matter, and hence the existence of quark stars, is for these reasons among the [[List of unsolved problems in physics|unsolved problems in physics]].
If these ideas are correct, quark stars might occur, and be observable, somewhere in the universe. Such a scenario is seen as scientifically plausible, but has not been proven observationally or experimentally; the very extreme conditions needed for stabilizing quark matter cannot be created in any laboratory and has not been observed directly in nature. The stability of quark matter, and hence the existence of quark stars, is for these reasons among the [[List of unsolved problems in physics|unsolved problems in physics]].


If quark stars can form, then the most likely place to find quark star matter would be inside [[neutron star]]s that exceed the internal pressure needed for [[degenerate matter|quark degeneracy]] – the point at which [[neutron]]s break down into a form of dense [[quark matter]]. They could also form if a [[massive star]] [[core collapse supernova|collapses]] at the end of its life, provided that it is possible for a star to be large enough to collapse beyond a neutron star but not large enough to form a [[black hole]].
If quark stars can form, then the most likely place to find quark star matter would be inside [[neutron star]]s that exceed the internal pressure needed for [[degenerate matter|quark degeneracy]] – the point at which [[neutron]]s break down into a form of dense quark matter. They could also form if a [[massive star]] [[core collapse supernova|collapses]] at the end of its life, provided that it is possible for a star to be large enough to collapse beyond a neutron star but not large enough to form a [[black hole]].


If they exist, quark stars would resemble and be easily mistaken for neutron stars: they would form in the death of a massive star in a [[Type II supernova]], be extremely dense and small, and possess a very high gravitational field. They would also lack some features of neutron stars, unless they also contained a shell of neutron matter, because free quarks are not expected to have properties matching degenerate neutron matter. For example, they might be radio-silent, or have atypical sizes, electromagnetic fields, or surface temperatures, compared to neutron stars.
If they exist, quark stars would resemble and be easily mistaken for neutron stars: they would form in the death of a massive star in a [[Type II supernova]], be extremely dense and small, and possess a very high gravitational field. They would also lack some features of neutron stars, unless they also contained a shell of neutron matter, because free quarks are not expected to have properties matching degenerate neutron matter. For example, they might be radio-silent, or have atypical sizes, electromagnetic fields, or surface temperatures, compared to neutron stars.
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The analysis about quark stars was first proposed in 1965 by Soviet physicists [[Dmitri Ivanenko|D. D. Ivanenko]] and [[D. F. Kurdgelaidze]].<ref>{{cite journal |title=Hypothesis concerning quark stars |last1=Ivanenko |first1=Dmitri D. |last2=Kurdgelaidze |first2=D. F. |journal=Astrophysics |volume=1 |issue=4 |pages=251–252 |date=1965 |bibcode=1965Ap......1..251I |doi=10.1007/BF01042830 |s2cid=119657479 }}</ref><ref>{{cite journal |title=Remarks on quark stars |last1=Ivanenko |first1=Dmitri D. |last2=Kurdgelaidze |first2=D. F. |journal=Lettere al Nuovo Cimento |volume=2 |pages=13–16 |date=1969 |bibcode=1969NCimL...2...13I |doi=10.1007/BF02753988|s2cid=120712416 }}</ref> Their existence has not been confirmed.
The analysis about quark stars was first proposed in 1965 by Soviet physicists [[Dmitri Ivanenko|D. D. Ivanenko]] and [[D. F. Kurdgelaidze]].<ref>{{cite journal |title=Hypothesis concerning quark stars |last1=Ivanenko |first1=Dmitri D. |last2=Kurdgelaidze |first2=D. F. |journal=Astrophysics |volume=1 |issue=4 |pages=251–252 |date=1965 |bibcode=1965Ap......1..251I |doi=10.1007/BF01042830 |s2cid=119657479 }}</ref><ref>{{cite journal |title=Remarks on quark stars |last1=Ivanenko |first1=Dmitri D. |last2=Kurdgelaidze |first2=D. F. |journal=Lettere al Nuovo Cimento |volume=2 |pages=13–16 |date=1969 |bibcode=1969NCimL...2...13I |doi=10.1007/BF02753988|s2cid=120712416 }}</ref> Their existence has not been confirmed.


The [[equation of state]] of [[quark matter]] is uncertain, as is the transition point between neutron-degenerate matter and quark matter. Theoretical uncertainties have precluded making predictions from [[first principles]]. Experimentally, the behaviour of quark matter is being actively studied with particle colliders, but this can only produce very hot (above 10<sup>12</sup>&nbsp;[[Kelvin (unit)|K]]) [[quark–gluon plasma]] blobs the size of atomic nuclei, which decay immediately after formation. The conditions inside compact stars with extremely high densities and temperatures well below 10<sup>12</sup>&nbsp;[[Kelvin (unit)|K]] cannot be recreated artificially, as there are no known methods to produce, store or study "cold" quark matter directly as it would be found inside quark stars. The theory predicts quark matter to possess some peculiar characteristics under these conditions.
The [[equation of state]] of [[quark matter]] is uncertain, as is the transition point between neutron-degenerate matter and quark matter.<ref>{{Cite journal |last=Mishra |first=H. |last2=Misra |first2=S.P. |last3=Panda |first3=P.K. |last4=Parida |first4=B.K. |date=1993 |title=NEUTRON MATTER – QUARK MATTER PHASE TRANSITION AND QUARK STAR |url=https://www.worldscientific.com/doi/abs/10.1142/S0218301393000212 |journal=International Journal of Modern Physics E |language=en |volume=02 |issue=03 |pages=547–563 |doi=10.1142/S0218301393000212 |issn=0218-3013|arxiv=nucl-th/9301003 }}</ref> Theoretical uncertainties have precluded making predictions from [[first principles]]. Experimentally, the behaviour of quark matter is being actively studied with particle colliders, but this can only produce very hot (above 10<sup>12</sup>&nbsp;[[Kelvin (unit)|K]]) [[quark–gluon plasma]] blobs the size of atomic nuclei, which decay immediately after formation. The conditions inside compact stars with extremely high densities and temperatures well below 10<sup>12</sup>&nbsp;[[Kelvin (unit)|K]] cannot be recreated artificially, as there are no known methods to produce, store or study "cold" quark matter directly as it would be found inside quark stars. The theory predicts quark matter to possess some peculiar characteristics under these conditions.{{citation needed|date=March 2024}}


==Formation==
==Formation==
[[File:TOV solution neutron quark star mass radius diagram.png|thumb|450px|TOV solution neutron quark star mass radius diagram{{clarify}}<ref>F. Douchin, P. Haensel, ''A unified equation of state of dense matter and neutron star structure'', "Astron. Astrophys." 380, 151 (2001).</ref>]]
[[File:TOV solution neutron quark star mass radius diagram.png|thumb|upright=1.75|Mass–radius relations for models of a neutron star with no exotic states (red) and a quark star (blue)<ref>F. Douchin, P. Haensel, ''A unified equation of state of dense matter and neutron star structure'', "Astron. Astrophys." 380, 151 (2001).</ref>]]
It is theorized that when the [[neutron-degenerate matter]], which makes up [[neutron star]]s, is put under sufficient pressure from the star's own [[gravity]] or the initial [[supernova]] creating it, the individual [[neutron]]s break down into their constituent [[quark]]s ([[up quark]]s and [[down quark]]s), forming what is known as [[quark matter]]. This conversion might be confined to the neutron star's center or it might transform the entire star, depending on the physical circumstances. Such a star is known as a quark star.<ref name="Shapiro">{{cite book |last1=Shapiro |first1=Stuart L. |last2=Teukolsky |first2=Saul A. |title=Black Holes, White Dwarfs and Neutron Stars: The Physics of Compact Objects |publisher=Wiley |year=2008 |isbn=978-0471873167}}</ref><ref>{{cite book |editor-last1=Blaschke |editor-first1=David |editor-first2=Armen |editor-last2=Sedrakian |editor-first3=Norman K. |editor-last3=Glendenning |title=Physics of neutron star interiors |series=Lecture Notes in Physics |volume=578 |publisher=Springer-Verlag |year=2001 |doi=10.1007/3-540-44578-1 |isbn=978-3-540-42340-9 }}</ref>
It is hypothesized that when the [[neutron-degenerate matter]], which makes up [[neutron star]]s, is put under sufficient pressure from the star's own [[gravity]] or the initial [[supernova]] creating it, the individual [[neutron]]s break down into their constituent [[quark]]s ([[up quark]]s and [[down quark]]s), forming what is known as quark matter. This conversion may be confined to the neutron star's center or it might transform the entire star, depending on the physical circumstances. Such a star is known as a quark star.<ref name="Shapiro">{{cite book |last1=Shapiro |first1=Stuart L. |last2=Teukolsky |first2=Saul A. |title=Black Holes, White Dwarfs and Neutron Stars: The Physics of Compact Objects |publisher=Wiley |year=2008 |isbn=978-0471873167}}</ref><ref>{{cite book |editor-last1=Blaschke |editor-first1=David |editor-first2=Armen |editor-last2=Sedrakian |editor-first3=Norman K. |editor-last3=Glendenning |title=Physics of Neutron Star Interiors |series=Lecture Notes in Physics |volume=578 |publisher=Springer-Verlag |year=2001 |doi=10.1007/3-540-44578-1 |isbn=978-3-540-42340-9 }}</ref>


===Stability and strange quark matter===
===Stability and strange quark matter===
Ordinary quark matter consisting of up and down quarks has a very high [[Fermi energy]] compared to ordinary atomic matter and is stable only under extreme temperatures and/or pressures. This suggests that the only stable quark stars will be neutron stars with a quark matter core, while quark stars consisting entirely of ordinary quark matter will be highly unstable and dissolve spontaneously.<ref name="Witten">{{cite journal |last1=Witten |first1=Edward |title=Cosmic separation of phases |journal=Physical Review D |volume=30 |issue=2 |pages=272–285 |date=1984 |doi=10.1103/PhysRevD.30.272 |bibcode=1984PhRvD..30..272W }}</ref><ref>{{cite journal |title=Strange matter |last1=Farhi |first1=Edward |last2=Jaffe |first2=Robert L. |journal=Physical Review D |volume=30 |issue= 11 |pages=2379 |date=1984 |bibcode=1984PhRvD..30.2379F |doi=10.1103/PhysRevD.30.2379}}</ref>
Ordinary quark matter consisting of up and down quarks has a very high [[Fermi energy]] compared to ordinary atomic matter and is stable only under extreme temperatures and/or pressures. This suggests that the only stable quark stars will be neutron stars with a quark matter core, while quark stars consisting entirely of ordinary quark matter will be highly unstable and re-arrange spontaneously.<ref name="Witten">{{cite journal |last1=Witten |first1=Edward |title=Cosmic separation of phases |journal=Physical Review D |volume=30 |issue=2 |pages=272–285 |date=1984 |doi=10.1103/PhysRevD.30.272 |bibcode=1984PhRvD..30..272W }}</ref><ref>{{cite journal |title=Strange matter |last1=Farhi |first1=Edward |last2=Jaffe |first2=Robert L. |journal=Physical Review D |volume=30 |issue= 11 |pages=2379 |date=1984 |bibcode=1984PhRvD..30.2379F |doi=10.1103/PhysRevD.30.2379}}</ref>


It has been shown that the high Fermi energy making ordinary quark matter unstable at low temperatures and pressures can be lowered substantially by the transformation of a sufficient number of up and down quarks into [[strange quark]]s, as strange quarks are, relatively speaking, a very heavy type of quark particle.<ref name="Witten" /> This kind of quark matter is known specifically as [[strange quark matter]] and it is speculated and subject to current scientific investigation whether it might in fact be stable under the conditions of interstellar space (i.e. near zero external pressure and temperature). If this is the case (known as the Bodmer–[[Edward Witten|Witten]] assumption), quark stars made entirely of quark matter would be stable if they quickly transform into strange quark matter.<ref name="Weber">{{Cite document |title=Strange-matter Stars |url=https://cds.cern.ch/record/278675 |last1=Weber |first1=Fridolin |last2=Kettner |first2=Christiane |last3=Weigel |first3=Manfred K. |last4=Glendenning |first4=Norman K. |journal= |access-date=2020-03-26 |archive-date=2022-03-22 |archive-url=https://web.archive.org/web/20220322124648/https://cds.cern.ch/record/278675 |url-status=live }} in {{cite book |title=International Symposium on Strangeness and Quark Matter, Kolymbari, Greece, 1-5 Sep 1994 |pages=308–317 |publisher=World Scientific |location=Singapore |editor-last1=Kumar |editor-first1=Shiva |editor-last2=Madsen |editor-first2=Jes |editor-last3=Panagiotou |editor-first3=Apostolos D. |editor-last4=Vassiliadis |editor-first4=G. }}</ref>
It has been shown that the high Fermi energy making ordinary quark matter unstable at low temperatures and pressures can be lowered substantially by the transformation of a sufficient number of up and down quarks into [[strange quark]]s, as strange quarks are, relatively speaking, a very heavy type of quark particle.<ref name="Witten" /> This kind of quark matter is known specifically as [[strange quark matter]] and it is speculated and subject to current scientific investigation whether it might in fact be stable under the conditions of interstellar space (i.e. near zero external pressure and temperature). If this is the case (known as the Bodmer–[[Edward Witten|Witten]] assumption), quark stars made entirely of quark matter would be stable if they quickly transform into strange quark matter.<ref name="Weber">{{Cite web|title=Strange-matter Stars |url=https://cds.cern.ch/record/278675 |last1=Weber |first1=Fridolin |last2=Kettner |first2=Christiane |last3=Weigel |first3=Manfred K. |last4=Glendenning |first4=Norman K. |journal= |date=1995 |access-date=2020-03-26 |archive-date=2022-03-22 |archive-url=https://web.archive.org/web/20220322124648/https://cds.cern.ch/record/278675 |url-status=live }} in {{cite book |title=International Symposium on Strangeness and Quark Matter, Kolymbari, Greece, 1-5 Sep 1994 |pages=308–317 |publisher=World Scientific |location=Singapore |editor-last1=Kumar |editor-first1=Shiva |editor-last2=Madsen |editor-first2=Jes |editor-last3=Panagiotou |editor-first3=Apostolos D. |editor-last4=Vassiliadis |editor-first4=G. }}</ref>


===Strange stars===
===Strange stars===
{{main|Strange star}}
{{main|Strange star}}
Quark stars made of [[strange quark matter]] are known as strange stars, and they form a subgroup under the quark star category.<ref name="Weber" />
Stars made of [[strange quark matter]] are known as strange stars. These form a distinct subtype of quark stars.<ref name="Weber" />


Theoretical investigations have revealed that quark stars might not only be produced from neutron stars and powerful supernovas, they could also be created in the early [[Chronology of the universe#Hadron epoch|cosmic phase separations]] following the [[Big Bang]].<ref name="Witten" /> If these primordial quark stars transform into strange quark matter before the external temperature and pressure conditions of the early Universe makes them unstable, they might turn out stable, if the Bodmer–Witten assumption holds true. Such primordial strange stars could survive to this day.<ref name="Witten" />
Theoretical investigations have revealed that quark stars might not only be produced from neutron stars and powerful supernovas, they could also be created in the early [[Chronology of the universe#Hadron epoch|cosmic phase separations]] following the [[Big Bang]].<ref name="Witten" /> If these primordial quark stars transform into strange quark matter before the external temperature and pressure conditions of the early Universe makes them unstable, they might turn out stable, if the Bodmer–Witten assumption holds true. Such primordial strange stars could survive to this day.<ref name="Witten" />


==Characteristics==
==Characteristics==
Quark stars have some special characteristics that separate them from ordinary neutron stars. Under the physical conditions found inside neutron stars, with extremely high densities but temperatures well below 10<sup>12</sup> K, quark matter is predicted to exhibit some peculiar characteristics. It is expected to behave as a [[Fermi liquid]] and enter a so-called color-flavor-locked (CFL) phase of [[color superconductivity]], where "color" refers to the six "charges" exhibited in the [[strong interaction]], instead of the two charges (positive and negative) in [[electromagnetism]]. At slightly lower densities, corresponding to higher layers closer to the surface of the compact star, the quark matter will behave as a non-CFL quark liquid, a phase that is even more mysterious than CFL and might include color conductivity and/or several additional yet undiscovered phases. None of these extreme conditions can currently be recreated in laboratories so nothing can be inferred about these phases from direct experiments.<ref>{{cite journal |last1=Alford |first1=Mark G. |last2=Schmitt |first2=Andreas |last3=Rajagopal |first3=Krishna |last4=Schäfer |first4=Thomas |title=Color superconductivity in dense quark matter |arxiv=0709.4635 |journal=Reviews of Modern Physics |volume=80 |issue=4 |pages=1455–1515 |year=2008 |doi=10.1103/RevModPhys.80.1455 |bibcode=2008RvMP...80.1455A |s2cid=14117263 }}</ref>
Quark stars have some special characteristics that separate them from ordinary neutron stars.

Under the physical conditions found inside neutron stars, with extremely high densities but temperatures well below 10<sup>12</sup> K, quark matter is predicted to exhibit some peculiar characteristics. It is expected to behave as a [[Fermi liquid]] and enter a so-called color-flavor-locked (CFL) phase of [[color superconductivity]], where "color" refers to the six "charges" exhibited in the [[strong interaction]], instead of the two charges (positive and negative) in [[electromagnetism]]. At slightly lower densities, corresponding to higher layers closer to the surface of the compact star, the quark matter will behave as a non-CFL quark liquid, a phase that is even more mysterious than CFL and might include color conductivity and/or several additional yet undiscovered phases. None of these extreme conditions can currently be recreated in laboratories so nothing can be inferred about these phases from direct experiments.<ref>{{cite journal |last1=Alford |first1=Mark G. |last2=Schmitt |first2=Andreas |last3=Rajagopal |first3=Krishna |last4=Schäfer |first4=Thomas |title=Color superconductivity in dense quark matter |arxiv=0709.4635 |journal=Reviews of Modern Physics |volume=80 |issue=4 |pages=1455–1515 |year=2008 |doi=10.1103/RevModPhys.80.1455 |bibcode=2008RvMP...80.1455A |s2cid=14117263 }}</ref>

If the conversion of neutron-degenerate matter to (strange) quark matter is total, a quark star can to some extent be imagined as a single gigantic [[hadron]]. But this "hadron" will be bound by gravity, rather than by the [[strong interaction|strong force]] that binds ordinary hadrons.


==Observed overdense neutron stars==
==Observed overdense neutron stars==
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A neutron star without deconfinement to quarks and higher densities cannot have a rotational period shorter than a millisecond; even with the unimaginable gravity of such a condensed object the centripetal force of faster rotation would eject matter from the surface, so detection of a pulsar of millisecond or less period would be strong evidence of a quark star.
A neutron star without deconfinement to quarks and higher densities cannot have a rotational period shorter than a millisecond; even with the unimaginable gravity of such a condensed object the centripetal force of faster rotation would eject matter from the surface, so detection of a pulsar of millisecond or less period would be strong evidence of a quark star.


Observations released by the [[Chandra X-ray Observatory]] on April 10, 2002 detected two possible quark stars, designated [[RX J1856.5-3754]] and [[3C 58]], which had previously been thought to be neutron stars. Based on the known laws of physics, the former appeared much smaller and the latter much colder than it should be, suggesting that they are composed of material denser than [[neutron-degenerate matter]]. However, these observations are met with skepticism by researchers who say the results were not conclusive;<ref name="Truemper2004">{{cite journal |last1=Trümper |first1=Joachim E. |last2=Burwitz |first2=Vadim |last3=Haberl |first3=Frank W. |last4=Zavlin |first4=Vyatcheslav E. |title=The puzzles of RX J1856.5-3754: neutron star or quark star? |journal=Nuclear Physics B: Proceedings Supplements |date=June 2004 |volume=132 |pages=560–565 |doi=10.1016/j.nuclphysbps.2004.04.094 |bibcode=2004NuPhS.132..560T |arxiv=astro-ph/0312600 |citeseerx=10.1.1.314.7466 |s2cid=425112 }}</ref> and since the late 2000s, the possibility that [[RX J1856.5-3754|RX J1856]] is a quark star has been excluded.
Observations released by the [[Chandra X-ray Observatory]] on April 10, 2002, detected two possible quark stars, designated [[RX J1856.5−3754]] and [[3C 58]], which had previously been thought to be neutron stars. Based on the known laws of physics, the former appeared much smaller and the latter much colder than it should be, suggesting that they are composed of material denser than [[neutron-degenerate matter]]. However, these observations are met with skepticism by researchers who say the results were not conclusive;<ref name="Truemper2004">{{cite journal |last1=Trümper |first1=Joachim E. |last2=Burwitz |first2=Vadim |last3=Haberl |first3=Frank W. |last4=Zavlin |first4=Vyatcheslav E. |title=The puzzles of RX J1856.5-3754: neutron star or quark star? |journal=Nuclear Physics B: Proceedings Supplements |date=June 2004 |volume=132 |pages=560–565 |doi=10.1016/j.nuclphysbps.2004.04.094 |bibcode=2004NuPhS.132..560T |arxiv=astro-ph/0312600 |citeseerx=10.1.1.314.7466 |s2cid=425112 }}</ref> and since the late 2000s, the possibility that [[RX J1856.5-3754|RX J1856]] is a quark star has been excluded.


Another star, [[XTE J1739-285]],<ref>Shiga, David; [https://www.newscientist.com/article/dn11221?DCMP=NLC-nletter&nsref=dn11221 "Fastest spinning star may have exotic heart"] {{Webarchive|url=https://web.archive.org/web/20120825035205/http://www.newscientist.com/article/dn11221?DCMP=NLC-nletter&nsref=dn11221 |date=2012-08-25 }}, ''New Scientist'', 2007 February 20</ref> has been observed by a team led by Philip Kaaret of the [[University of Iowa]] and reported as a possible quark star candidate.
Another star, [[XTE J1739-285]],<ref>Shiga, David; [https://www.newscientist.com/article/dn11221?DCMP=NLC-nletter&nsref=dn11221 "Fastest spinning star may have exotic heart"] {{Webarchive|url=https://web.archive.org/web/20120825035205/http://www.newscientist.com/article/dn11221?DCMP=NLC-nletter&nsref=dn11221 |date=2012-08-25 }}, ''New Scientist'', 2007 February 20</ref> has been observed by a team led by Philip Kaaret of the [[University of Iowa]] and reported as a possible quark star candidate.
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It was reported in 2008 that observations of supernovae [[SN 2006gy]], [[SN 2005gj]] and [[SN 2005ap]] also suggest the existence of quark stars.<ref>Chadha, Kulvinder Singh; [http://astronomynow.com/080604Secondsupernovaepointtoquarkstars.html "Second Supernovae Point to Quark Stars"] {{Webarchive|url=https://web.archive.org/web/20100125145543/http://astronomynow.com/080604Secondsupernovaepointtoquarkstars.html |date=2010-01-25 }}, ''Astronomy Now Online'', 2008 June 04</ref> It has been suggested that the collapsed core of supernova [[SN 1987A]] may be a quark star.<ref>{{cite journal |author1=Chan |author2=Cheng |author3=Harko |author4=Lau |author5=Lin |author6=Suen |author7=Tian |doi=10.1088/0004-637X/695/1/732 |journal=Astrophysical Journal |title=Could the compact remnant of SN 1987A be a quark star? |volume=695 |issue=1 |pages=732–746 |year=2009 |arxiv=0902.0653|bibcode = 2009ApJ...695..732C |s2cid=14402008 }}</ref><ref>Parsons, Paul; [https://www.newscientist.com/article/mg20126964.700-quark-star-may-hold-secret-to-early-universe.html "Quark star may hold secret to early universe"] {{Webarchive|url=https://web.archive.org/web/20150318100318/http://www.newscientist.com/article/mg20126964.700-quark-star-may-hold-secret-to-early-universe.html |date=2015-03-18 }}, ''New Scientist'', 2009 February 18</ref>
It was reported in 2008 that observations of supernovae [[SN 2006gy]], [[SN 2005gj]] and [[SN 2005ap]] also suggest the existence of quark stars.<ref>Chadha, Kulvinder Singh; [http://astronomynow.com/080604Secondsupernovaepointtoquarkstars.html "Second Supernovae Point to Quark Stars"] {{Webarchive|url=https://web.archive.org/web/20100125145543/http://astronomynow.com/080604Secondsupernovaepointtoquarkstars.html |date=2010-01-25 }}, ''Astronomy Now Online'', 2008 June 04</ref> It has been suggested that the collapsed core of supernova [[SN 1987A]] may be a quark star.<ref>{{cite journal |author1=Chan |author2=Cheng |author3=Harko |author4=Lau |author5=Lin |author6=Suen |author7=Tian |doi=10.1088/0004-637X/695/1/732 |journal=Astrophysical Journal |title=Could the compact remnant of SN 1987A be a quark star? |volume=695 |issue=1 |pages=732–746 |year=2009 |arxiv=0902.0653|bibcode = 2009ApJ...695..732C |s2cid=14402008 }}</ref><ref>Parsons, Paul; [https://www.newscientist.com/article/mg20126964.700-quark-star-may-hold-secret-to-early-universe.html "Quark star may hold secret to early universe"] {{Webarchive|url=https://web.archive.org/web/20150318100318/http://www.newscientist.com/article/mg20126964.700-quark-star-may-hold-secret-to-early-universe.html |date=2015-03-18 }}, ''New Scientist'', 2009 February 18</ref>


In 2015, Zi-Gao Dai et al. from Nanjing University suggested that Supernova [[ASASSN-15lh]] is a newborn strange quark star.<ref>{{Cite journal |title=The Most Luminous Supernova ASASSN-15lh: Signature of a Newborn Rapidly-Rotating Strange Quark Star |arxiv=1508.07745 |date=2015-08-31 |first1=Zi-Gao |last1=Dai |first2=Shan-Qin |last2=Wang |first3=J. S. |last3=Wang |first4=Ling-Jun |last4=Wang |first5=Yun-Wei |last5=Yu |doi=10.3847/0004-637X/817/2/132 |volume=817 |issue=2 |journal=The Astrophysical Journal |page=132 |bibcode=2016ApJ...817..132D |s2cid=54823427 }}</ref>
In 2015, Zi-Gao Dai et al. from Nanjing University suggested that Supernova [[ASASSN-15lh]] is a newborn strange quark star.<ref>{{Cite journal |title=The Most Luminous Supernova ASASSN-15lh: Signature of a Newborn Rapidly-Rotating Strange Quark Star |arxiv=1508.07745 |date=2015-08-31 |first1=Zi-Gao |last1=Dai |first2=Shan-Qin |last2=Wang |first3=J. S. |last3=Wang |first4=Ling-Jun |last4=Wang |first5=Yun-Wei |last5=Yu |doi=10.3847/0004-637X/817/2/132 |volume=817 |issue=2 |journal=The Astrophysical Journal |page=132 |bibcode=2016ApJ...817..132D |s2cid=54823427 |doi-access=free }}</ref>


In 2022 it was suggested that GW190425, which likely formed as a merger between two neutron stars giving off gravitational waves in the process, could be a quark star.<ref>{{cite web | url=https://www.space.com/strange-quark-stars-from-neutron-star-mergers | title=Strange quark star may have formed from a lucky cosmic merger | website=[[Space.com]] | date=16 September 2022 }}</ref>
In 2022 it was suggested that GW190425, which likely formed as a merger between two neutron stars giving off gravitational waves in the process, could be a quark star.<ref>{{cite web | url=https://www.space.com/strange-quark-stars-from-neutron-star-mergers | title=Strange quark star may have formed from a lucky cosmic merger | website=[[Space.com]] | date=16 September 2022 }}</ref>


==Other theorized quark formations==
==Other hypothesized quark formations==
{{more citations needed|date=December 2015}}
{{more citations needed|section|date=December 2015}}
Apart from ordinary quark matter and strange quark matter, other types of quark-gluon plasma might theoretically occur or be formed inside neutron stars and quark stars. This includes the following, some of which has been observed and studied in laboratories:
Apart from ordinary quark matter and strange quark matter, other types of quark-gluon plasma might hypothetically occur or be formed inside neutron stars and quark stars. This includes the following, some of which has been observed and studied in laboratories:


* Robert L. Jaffe 1977, suggested a [[tetraquark|four-quark]] state with strangeness (qs{{overline|qs}}).
* Robert L. Jaffe 1977, suggested a [[tetraquark|four-quark]] state with strangeness (qs{{overline|qs}}).
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* In 1987, a [[pentaquark]] state was first proposed with a charm anti-quark (qqqs{{overline|c}}).
* In 1987, a [[pentaquark]] state was first proposed with a charm anti-quark (qqqs{{overline|c}}).
* Pentaquark state with an antistrange quark and four light quarks consisting of up- and down-quarks only (qqqq{{overline|s}}).
* Pentaquark state with an antistrange quark and four light quarks consisting of up- and down-quarks only (qqqq{{overline|s}}).
* Light [[pentaquark]]s are grouped within an antidecuplet, the lightest candidate, Θ<sup>+</sup>, which can also be described by the diquark model of Robert L. Jaffe and Wilczek ([[Quantum chromodynamics|QCD]]).
* Light pentaquarks are grouped within an antidecuplet, the lightest candidate, Θ<sup>+</sup>, which can also be described by the diquark model of Robert L. Jaffe and Wilczek ([[Quantum chromodynamics|QCD]]).
* [[pentaquark|Θ]]<sup>++</sup> and antiparticle {{overline|Θ}}<sup>−−</sup>.
* [[pentaquark|Θ]]<sup>++</sup> and antiparticle {{overline|Θ}}<sup>−−</sup>.
* Doubly strange [[pentaquark]] (ssdd{{overline|u}}), member of the light pentaquark antidecuplet.
* Doubly strange pentaquark (ssdd{{overline|u}}), member of the light pentaquark antidecuplet.
* Charmed [[pentaquark]] Θ<sub>c</sub>(3100) (uudd{{overline|c}}) state was detected by the H1 collaboration.<ref name="H1">{{cite journal |author1=H1 Collaboration |doi=10.1016/j.physletb.2004.03.012 |journal=Physics Letters B |last2=Aktas |first2=A. |last3=Andreev |first3=V. |last4=Anthonis |first4=T. |last5=Asmone |first5=A. |last6=Babaev |first6=A. |last7=Backovic |first7=S. |last8=Bähr |first8=J. |last9=Baranov |first9=P. |display-authors=6 |title=Evidence for a narrow anti-charmed baryon state of mass |volume=588 |issue=1–2 |pages=17–28 |year=2004 |arxiv=hep-ex/0403017 |bibcode=2004PhLB..588...17A |s2cid=119375207 }}</ref>
* Charmed pentaquark Θ<sub>c</sub>(3100) (uudd{{overline|c}}) state was detected by the H1 collaboration.<ref name="H1">{{cite journal |author1=H1 Collaboration |doi=10.1016/j.physletb.2004.03.012 |journal=Physics Letters B |last2=Aktas |first2=A. |last3=Andreev |first3=V. |last4=Anthonis |first4=T. |last5=Asmone |first5=A. |last6=Babaev |first6=A. |last7=Backovic |first7=S. |last8=Bähr |first8=J. |last9=Baranov |first9=P. |display-authors=6 |title=Evidence for a narrow anti-charmed baryon state of mass |volume=588 |issue=1–2 |pages=17–28 |year=2004 |arxiv=hep-ex/0403017 |bibcode=2004PhLB..588...17A |s2cid=119375207 }}</ref>
* Tetraquark particles might form inside neutron stars and under other extreme conditions. In 2008, 2013 and 2014 the tetraquark particle of Z(4430), was discovered and investigated in laboratories on [[Earth]].<ref>{{cite web |url=http://www.universetoday.com/111110/how-cerns-discovery-of-exotic-particles-may-affect-astrophysics |title=How CERN's discovery of exotic particles may affect astrophysics |last=Koberlein |first=Brian |publisher=Universe Today |date=10 April 2014 |access-date=14 April 2014 |archive-date=14 April 2014 |archive-url=https://web.archive.org/web/20140414053520/http://www.universetoday.com/111110/how-cerns-discovery-of-exotic-particles-may-affect-astrophysics/ |url-status=live }}/</ref>
* Tetraquark particles might form inside neutron stars and under other extreme conditions. In 2008, 2013 and 2014 the tetraquark particle of [[Z(4430)]], was discovered and investigated in laboratories on [[Earth]].<ref>{{cite web |url=http://www.universetoday.com/111110/how-cerns-discovery-of-exotic-particles-may-affect-astrophysics |title=How CERN's discovery of exotic particles may affect astrophysics |last=Koberlein |first=Brian |publisher=Universe Today |date=10 April 2014 |access-date=14 April 2014 |archive-date=14 April 2014 |archive-url=https://web.archive.org/web/20140414053520/http://www.universetoday.com/111110/how-cerns-discovery-of-exotic-particles-may-affect-astrophysics/ |url-status=live }}/</ref>


==See also==
==See also==
{{Portal|Physics|Astronomy}}
{{cmn|
<!-- alphabetical order please [[WP:SEEALSO]] -->
* [[Planck star]]
<!-- please add a short description [[WP:SEEALSO]], via {{subst:AnnotatedListOfLinks}} or {{Annotated link}} -->
* [[Quark-nova]]
{{div col|colwidth=20em|small=yes}}
* [[Quantum chromodynamics]]
* {{Annotated link |Deconfinement}}
* [[Neutron stars]] – [[neutron matter]] – [[degenerate matter|neutron-degenerate matter]] – [[neutron]]
* {{Annotated link |Neutron}}
* [[Deconfinement]]
** {{Annotated link |Neutron matter}}
* [[Tolman–Oppenheimer–Volkoff limit]] on the mass of a neutron star.
** {{Annotated link |Neutron stars}}

* [[Compact star]]
* {{Annotated link |Planck star}}
* {{Annotated link |Quark-nova}}
** [[Exotic star]]
* {{Annotated link |Quantum chromodynamics}}
** [[Neutron star]]
* {{Annotated link |Tolman–Oppenheimer–Volkoff limit}}
** [[Pulsar]]
* {{Annotated link |Degenerate matter}}
** [[Magnetar]]
** {{Annotated link |Neutron matter}}
** [[White dwarf]]
** {{Annotated link |Preon matter}}
** [[Stellar black hole]]
** {{Annotated link |QCD matter}}

** {{Annotated link |Quark–gluon plasma}}
* [[Degenerate matter]]
** [[QCD matter]]
** {{Annotated link |Quark matter}}
** {{Annotated link |Strangelet}}
** [[Quark–gluon plasma]]
* {{Annotated link |Compact star}}
** [[Strangelet]]
** {{Annotated link |Exotic star}}
** [[Quark matter]]
** {{Annotated link |Magnetar}}
** [[Neutronium]]
** {{Annotated link |Neutron star}}
** [[Preon matter]]
** {{Annotated link |Pulsar}}
}}
** {{Annotated link |Stellar black hole}}
** {{Annotated link |White dwarf}}
{{div col end}}
<!-- alphabetical order please [[WP:SEEALSO]] -->


==References==
==References==
Line 102: Line 103:


==Sources and further reading==
==Sources and further reading==
* {{cite book |editor-last1=Blaschke |editor-first1=David |editor-last2=Sedrakian |editor-first2=David |title=Superdense QCD Matter and Compact Stars |series=NATO Science Series II: Mathematics, Physics and Chemistry |volume=197 |publisher=Springer |year=2003 |doi=10.1007/1-4020-3430-X |isbn=978-1-4020-3428-2 |url=http://cds.cern.ch/record/1338948 }}
* {{cite book |editor-last1=Blaschke |editor-first1=David |editor-last2=Sedrakian |editor-first2=David |title=Superdense QCD Matter and Compact Stars |series=NATO Science Series II: Mathematics, Physics and Chemistry |volume=197 |publisher=Springer |year=2003 |doi=10.1007/1-4020-3430-X |isbn=978-1-4020-3428-2 |url=https://cds.cern.ch/record/1338948 }}
* {{cite book |editor-last1=Blaschke |editor-first1=David |editor-first2=Armen |editor-last2=Sedrakian |editor-first3=Norman K. |editor-last3=Glendenning |title=Physics of neutron star interiors |series=Lecture Notes in Physics |volume=578 |publisher=Springer-Verlag |year=2001 |doi=10.1007/3-540-44578-1 |isbn=978-3-540-42340-9 }}
* {{cite book |editor-last1=Blaschke |editor-first1=David |editor-first2=Armen |editor-last2=Sedrakian |editor-first3=Norman K. |editor-last3=Glendenning |title=Physics of Neutron Star Interiors |series=Lecture Notes in Physics |volume=578 |publisher=Springer-Verlag |year=2001 |doi=10.1007/3-540-44578-1 |isbn=978-3-540-42340-9 }}
* {{cite book |editor-last1=Plessas |editor-first1=Willibald |editor-last2=Mathelitsch |editor-first2=Leopold |url=https://searchworks.stanford.edu/view/4788102 |title=Lectures on quark matter |series=Lecture Notes in Physics |volume=583 |publisher=Springer |year=2002 |doi=10.1007/3-540-45792-5 |isbn=978-3-540-43234-0 }}
* {{cite book |editor-last1=Plessas |editor-first1=Willibald |editor-last2=Mathelitsch |editor-first2=Leopold |url=https://searchworks.stanford.edu/view/4788102 |title=Lectures on Quark Matter |series=Lecture Notes in Physics |volume=583 |publisher=Springer |year=2002 |doi=10.1007/3-540-45792-5 |isbn=978-3-540-43234-0 }}


==External links==
==External links==
*{{cite journal |last1=Jaffe |first1=Robert L. |title=Perhaps a Stable Dihyperon |journal=Physical Review Letters |volume=38 |issue=5 |pages=195–198 |date=1977 |doi=10.1103/PhysRevLett.38.195|bibcode = 1977PhRvL..38..195J |osti=1446298 |url=https://www.slac.stanford.edu/cgi-bin/getdoc/slac-pub-1828.pdf }}
*{{cite journal |last1=Jaffe |first1=Robert L. |title=Perhaps a Stable Dihyperon |journal=Physical Review Letters |volume=38 |issue=5 |pages=195–198 |date=1977 |doi=10.1103/PhysRevLett.38.195|bibcode = 1977PhRvL..38..195J |osti=1446298 |url=https://www.slac.stanford.edu/cgi-bin/getdoc/slac-pub-1828.pdf }}
*[http://chandra.harvard.edu/photo/2002/0211/0211_illustration_300.jpg Neutron Star/Quark Star Interior (image to print)]
*[http://chandra.harvard.edu/photo/2002/0211/0211_illustration_300.jpg Neutron Star/Quark Star Interior (image to print)]
*Whitfield,John; [http://www.nature.com/news/2002/020411/full/news020408-8.html "Quark star glimmers"], ''[[Nature (journal)|Nature]]'', 2002 April 11
*Whitfield, John; [http://www.nature.com/news/2002/020411/full/news020408-8.html "Quark star glimmers"], ''[[Nature (journal)|Nature]]'', 2002 April 11
*[https://cerncourier.com/a/debate-sparked-on-quark-stars/ "Debate sparked on quark stars"], ''CERN Courier'' '''42''', #5, June 2002, [https://cds.cern.ch/record/1733341 page 13]
*[https://cerncourier.com/a/debate-sparked-on-quark-stars/ "Debate sparked on quark stars"], ''CERN Courier'' '''42''', #5, June 2002, [https://cds.cern.ch/record/1733341 page 13]
*Beck, Paul; [https://web.archive.org/web/20060313223759/http://www.popsci.com/popsci/aviationspace/a6885b4a1db84010vgnvcm1000004eecbccdrcrd.html "Wish Upon a Quark Star"], ''Popular Science'', June 2002
*Beck, Paul; [https://web.archive.org/web/20060313223759/http://www.popsci.com/popsci/aviationspace/a6885b4a1db84010vgnvcm1000004eecbccdrcrd.html "Wish Upon a Quark Star"], ''Popular Science'', June 2002
*{{cite journal |author1=Drake |author2=Marshall |author3=Dreizler |author4=Freeman |author5=Fruscione |author6=Juda |author7=Kashyap |author8=Nicastro |author9=Pease |display-authors=8 |doi=10.1086/340368 |journal=Astrophysical Journal |volume=572 |title=Is RX J185635-375 a Quark Star? |issue=2 |pages=996–1001 |date=2002 |arxiv=astro-ph/0204159 |bibcode = 2002ApJ...572..996D |s2cid=18481546 }}
*{{cite journal |author1=Drake |author2=Marshall |author3=Dreizler |author4=Freeman |author5=Fruscione |author6=Juda |author7=Kashyap |author8=Nicastro |author9=Pease |display-authors=8 |doi=10.1086/340368 |journal=Astrophysical Journal |volume=572 |title=Is RX J185635-375 a Quark Star? |issue=2 |pages=996–1001 |date=2002 |arxiv=astro-ph/0204159 |bibcode = 2002ApJ...572..996D |s2cid=18481546 }}
*Krivoruchenko, M. I.; [http://www.jetpletters.ac.ru/ps/1224/article_18487.shtml "Strange, quark, and metastable neutron stars"] {{Webarchive|url=https://web.archive.org/web/20131016114425/http://www.jetpletters.ac.ru/ps/1224/article_18487.shtml |date=2013-10-16 }}, JETP Letters, vol. 46, no. 1, 10 July 1987, pages 3-6 (page 6: Perhaps a 1,700-year-old quark star in SNR MSH 15-52)
*Krivoruchenko, M. I.; [http://www.jetpletters.ac.ru/ps/1224/article_18487.shtml "Strange, quark, and metastable neutron stars"] {{Webarchive|url=https://web.archive.org/web/20131016114425/http://www.jetpletters.ac.ru/ps/1224/article_18487.shtml |date=2013-10-16 }}, JETP Letters, vol. 46, no. 1, 10 July 1987, pages 3–6 (page 6: Perhaps a 1,700-year-old quark star in SNR MSH 15–52)
*Rothstein, Dave; [https://web.archive.org/web/20030418110053/http://curious.astro.cornell.edu/question.php?number=445 "Curious About Astronomy: What process would bring about a quark star?"], question #445, January 2003
*Rothstein, Dave; [https://web.archive.org/web/20030418110053/http://curious.astro.cornell.edu/question.php?number=445 "Curious About Astronomy: What process would bring about a quark star?"], question #445, January 2003
*Nemiroff, Robert; Bonnell, Jerry; [http://antwrp.gsfc.nasa.gov/apod/ap020414.html "RX J185635-375: Candidate Quark Star"], ''Astronomy Picture of the Day'', NASA Goddard Space Flight Center, 2002 April 14
*Nemiroff, Robert; Bonnell, Jerry; [http://antwrp.gsfc.nasa.gov/apod/ap020414.html "RX J185635-375: Candidate Quark Star"], ''Astronomy Picture of the Day'', NASA Goddard Space Flight Center, 2002 April 14
Line 125: Line 126:
*Cramer, John G.: [http://www.npl.washington.edu/AV/altvw114.html "Quark Stars, Alternate View Column AV-114"], ''Analog Science Fiction & Fact Magazine'', November 2002
*Cramer, John G.: [http://www.npl.washington.edu/AV/altvw114.html "Quark Stars, Alternate View Column AV-114"], ''Analog Science Fiction & Fact Magazine'', November 2002


{{Portal bar|Astronomy|Spaceflight|Outer space|Solar System}}
{{neutron star}}
{{neutron star}}
{{Star}}
{{Star}}
{{Supernovae}}
{{Supernovae}}

{{Portal bar|Astronomy|Spaceflight|Outer space|Solar System}}
{{DEFAULTSORT:Quark Star}}
{{DEFAULTSORT:Quark Star}}
[[Category:Star types]]
[[Category:Star types]]

Latest revision as of 18:34, 5 December 2024

A quark star is a hypothetical type of compact, exotic star, where extremely high core temperature and pressure have forced nuclear particles to form quark matter, a continuous state of matter consisting of free quarks.[1]

Background

[edit]

Some massive stars collapse to form neutron stars at the end of their life cycle, as has been both observed and explained theoretically. Under the extreme temperatures and pressures inside neutron stars, the neutrons are normally kept apart by a degeneracy pressure, stabilizing the star and hindering further gravitational collapse.[2] However, it is hypothesized that under even more extreme temperature and pressure, the degeneracy pressure of the neutrons is overcome, and the neutrons are forced to merge and dissolve into their constituent quarks, creating an ultra-dense phase of quark matter based on densely packed quarks. In this state, a new equilibrium is supposed to emerge, as a new degeneracy pressure between the quarks, as well as repulsive electromagnetic forces, will occur and hinder total gravitational collapse.

If these ideas are correct, quark stars might occur, and be observable, somewhere in the universe. Such a scenario is seen as scientifically plausible, but has not been proven observationally or experimentally; the very extreme conditions needed for stabilizing quark matter cannot be created in any laboratory and has not been observed directly in nature. The stability of quark matter, and hence the existence of quark stars, is for these reasons among the unsolved problems in physics.

If quark stars can form, then the most likely place to find quark star matter would be inside neutron stars that exceed the internal pressure needed for quark degeneracy – the point at which neutrons break down into a form of dense quark matter. They could also form if a massive star collapses at the end of its life, provided that it is possible for a star to be large enough to collapse beyond a neutron star but not large enough to form a black hole.

If they exist, quark stars would resemble and be easily mistaken for neutron stars: they would form in the death of a massive star in a Type II supernova, be extremely dense and small, and possess a very high gravitational field. They would also lack some features of neutron stars, unless they also contained a shell of neutron matter, because free quarks are not expected to have properties matching degenerate neutron matter. For example, they might be radio-silent, or have atypical sizes, electromagnetic fields, or surface temperatures, compared to neutron stars.

History

[edit]

The analysis about quark stars was first proposed in 1965 by Soviet physicists D. D. Ivanenko and D. F. Kurdgelaidze.[3][4] Their existence has not been confirmed.

The equation of state of quark matter is uncertain, as is the transition point between neutron-degenerate matter and quark matter.[5] Theoretical uncertainties have precluded making predictions from first principles. Experimentally, the behaviour of quark matter is being actively studied with particle colliders, but this can only produce very hot (above 1012 K) quark–gluon plasma blobs the size of atomic nuclei, which decay immediately after formation. The conditions inside compact stars with extremely high densities and temperatures well below 1012 K cannot be recreated artificially, as there are no known methods to produce, store or study "cold" quark matter directly as it would be found inside quark stars. The theory predicts quark matter to possess some peculiar characteristics under these conditions.[citation needed]

Formation

[edit]
Mass–radius relations for models of a neutron star with no exotic states (red) and a quark star (blue)[6]

It is hypothesized that when the neutron-degenerate matter, which makes up neutron stars, is put under sufficient pressure from the star's own gravity or the initial supernova creating it, the individual neutrons break down into their constituent quarks (up quarks and down quarks), forming what is known as quark matter. This conversion may be confined to the neutron star's center or it might transform the entire star, depending on the physical circumstances. Such a star is known as a quark star.[7][8]

Stability and strange quark matter

[edit]

Ordinary quark matter consisting of up and down quarks has a very high Fermi energy compared to ordinary atomic matter and is stable only under extreme temperatures and/or pressures. This suggests that the only stable quark stars will be neutron stars with a quark matter core, while quark stars consisting entirely of ordinary quark matter will be highly unstable and re-arrange spontaneously.[9][10]

It has been shown that the high Fermi energy making ordinary quark matter unstable at low temperatures and pressures can be lowered substantially by the transformation of a sufficient number of up and down quarks into strange quarks, as strange quarks are, relatively speaking, a very heavy type of quark particle.[9] This kind of quark matter is known specifically as strange quark matter and it is speculated and subject to current scientific investigation whether it might in fact be stable under the conditions of interstellar space (i.e. near zero external pressure and temperature). If this is the case (known as the Bodmer–Witten assumption), quark stars made entirely of quark matter would be stable if they quickly transform into strange quark matter.[11]

Strange stars

[edit]

Stars made of strange quark matter are known as strange stars. These form a distinct subtype of quark stars.[11]

Theoretical investigations have revealed that quark stars might not only be produced from neutron stars and powerful supernovas, they could also be created in the early cosmic phase separations following the Big Bang.[9] If these primordial quark stars transform into strange quark matter before the external temperature and pressure conditions of the early Universe makes them unstable, they might turn out stable, if the Bodmer–Witten assumption holds true. Such primordial strange stars could survive to this day.[9]

Characteristics

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Quark stars have some special characteristics that separate them from ordinary neutron stars. Under the physical conditions found inside neutron stars, with extremely high densities but temperatures well below 1012 K, quark matter is predicted to exhibit some peculiar characteristics. It is expected to behave as a Fermi liquid and enter a so-called color-flavor-locked (CFL) phase of color superconductivity, where "color" refers to the six "charges" exhibited in the strong interaction, instead of the two charges (positive and negative) in electromagnetism. At slightly lower densities, corresponding to higher layers closer to the surface of the compact star, the quark matter will behave as a non-CFL quark liquid, a phase that is even more mysterious than CFL and might include color conductivity and/or several additional yet undiscovered phases. None of these extreme conditions can currently be recreated in laboratories so nothing can be inferred about these phases from direct experiments.[12]

Observed overdense neutron stars

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At least under the assumptions mentioned above, the probability of a given neutron star being a quark star is low,[citation needed] so in the Milky Way there would only be a small population of quark stars. If it is correct, however, that overdense neutron stars can turn into quark stars, that makes the possible number of quark stars higher than was originally thought, as observers would be looking for the wrong type of star.[citation needed]

A neutron star without deconfinement to quarks and higher densities cannot have a rotational period shorter than a millisecond; even with the unimaginable gravity of such a condensed object the centripetal force of faster rotation would eject matter from the surface, so detection of a pulsar of millisecond or less period would be strong evidence of a quark star.

Observations released by the Chandra X-ray Observatory on April 10, 2002, detected two possible quark stars, designated RX J1856.5−3754 and 3C 58, which had previously been thought to be neutron stars. Based on the known laws of physics, the former appeared much smaller and the latter much colder than it should be, suggesting that they are composed of material denser than neutron-degenerate matter. However, these observations are met with skepticism by researchers who say the results were not conclusive;[13] and since the late 2000s, the possibility that RX J1856 is a quark star has been excluded.

Another star, XTE J1739-285,[14] has been observed by a team led by Philip Kaaret of the University of Iowa and reported as a possible quark star candidate.

In 2006, You-Ling Yue et al., from Peking University, suggested that PSR B0943+10 may in fact be a low-mass quark star.[15]

It was reported in 2008 that observations of supernovae SN 2006gy, SN 2005gj and SN 2005ap also suggest the existence of quark stars.[16] It has been suggested that the collapsed core of supernova SN 1987A may be a quark star.[17][18]

In 2015, Zi-Gao Dai et al. from Nanjing University suggested that Supernova ASASSN-15lh is a newborn strange quark star.[19]

In 2022 it was suggested that GW190425, which likely formed as a merger between two neutron stars giving off gravitational waves in the process, could be a quark star.[20]

Other hypothesized quark formations

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Apart from ordinary quark matter and strange quark matter, other types of quark-gluon plasma might hypothetically occur or be formed inside neutron stars and quark stars. This includes the following, some of which has been observed and studied in laboratories:

  • Robert L. Jaffe 1977, suggested a four-quark state with strangeness (qsqs).
  • Robert L. Jaffe 1977 suggested the H dibaryon, a six-quark state with equal numbers of up-, down-, and strange quarks (represented as uuddss or udsuds).
  • Bound multi-quark systems with heavy quarks (QQqq).
  • In 1987, a pentaquark state was first proposed with a charm anti-quark (qqqsc).
  • Pentaquark state with an antistrange quark and four light quarks consisting of up- and down-quarks only (qqqqs).
  • Light pentaquarks are grouped within an antidecuplet, the lightest candidate, Θ+, which can also be described by the diquark model of Robert L. Jaffe and Wilczek (QCD).
  • Θ++ and antiparticle Θ−−.
  • Doubly strange pentaquark (ssddu), member of the light pentaquark antidecuplet.
  • Charmed pentaquark Θc(3100) (uuddc) state was detected by the H1 collaboration.[21]
  • Tetraquark particles might form inside neutron stars and under other extreme conditions. In 2008, 2013 and 2014 the tetraquark particle of Z(4430), was discovered and investigated in laboratories on Earth.[22]

See also

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  • Deconfinement – Phase of matter where certain particles can exist outside of a bound state
  • Neutron – Subatomic particle with no charge
    • Neutron matter – Type of dense exotic matter in physics
    • Neutron stars – Collapsed core of a massive star
  • Planck star – Hypothetical astronomical object
  • Quark-nova – Hypothetical violent explosion resulting from conversion of a neutron star to a quark star
  • Quantum chromodynamics – Theory of the strong nuclear interactions
  • Tolman–Oppenheimer–Volkoff limit – Upper bound to the mass of cold, nonrotating neutron stars
  • Degenerate matter – Type of dense exotic matter in physics
    • Neutron matter – Type of dense exotic matter in physics
    • Preon matter – Hypothetical subatomic particle
    • QCD matter – Hypothetical phases of matter
    • Quark–gluon plasma – Phase of quantum chromodynamics (QCD)
    • Quark matter – Hypothetical phases of matter
    • Strangelet – Type of hypothetical particle
  • Compact star – Classification in astronomy
    • Exotic star – Hypothetical types of stars
    • Magnetar – Type of neutron star with a strong magnetic field
    • Neutron star – Collapsed core of a massive star
    • Pulsar – Rapidly rotating neutron star
    • Stellar black hole – Black hole formed by a collapsed star
    • White dwarf – Type of stellar remnant composed mostly of electron-degenerate matter

References

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  1. ^ Sutter, Paul (5 October 2023). "These Stars Are Like Nothing Else You'll Ever See". Popular Mechanics. Retrieved 6 July 2024.
  2. ^ Seife, Charles. "Quark Stars Get Real". Science.org.
  3. ^ Ivanenko, Dmitri D.; Kurdgelaidze, D. F. (1965). "Hypothesis concerning quark stars". Astrophysics. 1 (4): 251–252. Bibcode:1965Ap......1..251I. doi:10.1007/BF01042830. S2CID 119657479.
  4. ^ Ivanenko, Dmitri D.; Kurdgelaidze, D. F. (1969). "Remarks on quark stars". Lettere al Nuovo Cimento. 2: 13–16. Bibcode:1969NCimL...2...13I. doi:10.1007/BF02753988. S2CID 120712416.
  5. ^ Mishra, H.; Misra, S.P.; Panda, P.K.; Parida, B.K. (1993). "NEUTRON MATTER – QUARK MATTER PHASE TRANSITION AND QUARK STAR". International Journal of Modern Physics E. 02 (03): 547–563. arXiv:nucl-th/9301003. doi:10.1142/S0218301393000212. ISSN 0218-3013.
  6. ^ F. Douchin, P. Haensel, A unified equation of state of dense matter and neutron star structure, "Astron. Astrophys." 380, 151 (2001).
  7. ^ Shapiro, Stuart L.; Teukolsky, Saul A. (2008). Black Holes, White Dwarfs and Neutron Stars: The Physics of Compact Objects. Wiley. ISBN 978-0471873167.
  8. ^ Blaschke, David; Sedrakian, Armen; Glendenning, Norman K., eds. (2001). Physics of Neutron Star Interiors. Lecture Notes in Physics. Vol. 578. Springer-Verlag. doi:10.1007/3-540-44578-1. ISBN 978-3-540-42340-9.
  9. ^ a b c d Witten, Edward (1984). "Cosmic separation of phases". Physical Review D. 30 (2): 272–285. Bibcode:1984PhRvD..30..272W. doi:10.1103/PhysRevD.30.272.
  10. ^ Farhi, Edward; Jaffe, Robert L. (1984). "Strange matter". Physical Review D. 30 (11): 2379. Bibcode:1984PhRvD..30.2379F. doi:10.1103/PhysRevD.30.2379.
  11. ^ a b Weber, Fridolin; Kettner, Christiane; Weigel, Manfred K.; Glendenning, Norman K. (1995). "Strange-matter Stars". Archived from the original on 2022-03-22. Retrieved 2020-03-26. in Kumar, Shiva; Madsen, Jes; Panagiotou, Apostolos D.; Vassiliadis, G. (eds.). International Symposium on Strangeness and Quark Matter, Kolymbari, Greece, 1-5 Sep 1994. Singapore: World Scientific. pp. 308–317.
  12. ^ Alford, Mark G.; Schmitt, Andreas; Rajagopal, Krishna; Schäfer, Thomas (2008). "Color superconductivity in dense quark matter". Reviews of Modern Physics. 80 (4): 1455–1515. arXiv:0709.4635. Bibcode:2008RvMP...80.1455A. doi:10.1103/RevModPhys.80.1455. S2CID 14117263.
  13. ^ Trümper, Joachim E.; Burwitz, Vadim; Haberl, Frank W.; Zavlin, Vyatcheslav E. (June 2004). "The puzzles of RX J1856.5-3754: neutron star or quark star?". Nuclear Physics B: Proceedings Supplements. 132: 560–565. arXiv:astro-ph/0312600. Bibcode:2004NuPhS.132..560T. CiteSeerX 10.1.1.314.7466. doi:10.1016/j.nuclphysbps.2004.04.094. S2CID 425112.
  14. ^ Shiga, David; "Fastest spinning star may have exotic heart" Archived 2012-08-25 at the Wayback Machine, New Scientist, 2007 February 20
  15. ^ Yue, You-Ling; Cui, Xiao-Hong; Xu, Ren-Xin (2006). "Is PSR B0943+10 a low-mass quark star?". Astrophysical Journal. 649 (2): L95 – L98. arXiv:astro-ph/0603468. Bibcode:2006ApJ...649L..95Y. doi:10.1086/508421. S2CID 18183996.
  16. ^ Chadha, Kulvinder Singh; "Second Supernovae Point to Quark Stars" Archived 2010-01-25 at the Wayback Machine, Astronomy Now Online, 2008 June 04
  17. ^ Chan; Cheng; Harko; Lau; Lin; Suen; Tian (2009). "Could the compact remnant of SN 1987A be a quark star?". Astrophysical Journal. 695 (1): 732–746. arXiv:0902.0653. Bibcode:2009ApJ...695..732C. doi:10.1088/0004-637X/695/1/732. S2CID 14402008.
  18. ^ Parsons, Paul; "Quark star may hold secret to early universe" Archived 2015-03-18 at the Wayback Machine, New Scientist, 2009 February 18
  19. ^ Dai, Zi-Gao; Wang, Shan-Qin; Wang, J. S.; Wang, Ling-Jun; Yu, Yun-Wei (2015-08-31). "The Most Luminous Supernova ASASSN-15lh: Signature of a Newborn Rapidly-Rotating Strange Quark Star". The Astrophysical Journal. 817 (2): 132. arXiv:1508.07745. Bibcode:2016ApJ...817..132D. doi:10.3847/0004-637X/817/2/132. S2CID 54823427.
  20. ^ "Strange quark star may have formed from a lucky cosmic merger". Space.com. 16 September 2022.
  21. ^ H1 Collaboration; Aktas, A.; Andreev, V.; Anthonis, T.; Asmone, A.; Babaev, A.; et al. (2004). "Evidence for a narrow anti-charmed baryon state of mass". Physics Letters B. 588 (1–2): 17–28. arXiv:hep-ex/0403017. Bibcode:2004PhLB..588...17A. doi:10.1016/j.physletb.2004.03.012. S2CID 119375207.{{cite journal}}: CS1 maint: numeric names: authors list (link)
  22. ^ Koberlein, Brian (10 April 2014). "How CERN's discovery of exotic particles may affect astrophysics". Universe Today. Archived from the original on 14 April 2014. Retrieved 14 April 2014./

Sources and further reading

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