Cosmic string: Difference between revisions

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{{short description|Speculative feature of the early universe}}
{{distinguish|text=[[String (physics)]], the subject of [[string theory]]}}
'''Cosmic strings''' are hypothetical 1-dimensional [[topological defect]]s which may have formed during a [[Symmetry breaking|symmetry-breaking]] [[cosmological phase transition|phase transition]] in the early universe when the [[topology]] of the [[Vacuum state|vacuum]] manifold associated to this symmetry breaking was not [[Simply connected space|simply connected]]. Their existence was first contemplated by the theoretical physicist [[Tom Kibble]] in the 1970s.<ref name="Kibble 1976">{{cite journal |doi=10.1088/0305-4470/9/8/029 |title=Topology of cosmic domains and strings |year=1976 |last1=Kibble |first1=Tom W K |journal= Journal of Physics A: Mathematical and General |volume=9 |issue=8 |pages=1387–1398 |bibcode=1976JPhA....9.1387K }}</ref>
{{Technical|date=May 2021}}
 
'''Cosmic strings''' are hypothetical 1-dimensional [[topological defect]]s which may have formed during a [[Symmetry breaking|symmetry-breaking]] [[cosmological phase transition|phase transition]] in the early universe when the [[topology]] of the [[Vacuum state|vacuum]] manifold associated to this symmetry breaking was not [[Simply connected space|simply connected]]. Their existence was first contemplated by the theoretical physicist [[Tom Kibble]] in the 1970s.<ref name="Kibble 1976">{{cite journal |doi=10.1088/0305-4470/9/8/029 |title=Topology of cosmic domains and strings |year=1976 |last1=Kibble |first1=Tom W K |journal= Journal of Physics A: Mathematical and General |volume=9 |issue=8 |pages=1387–1398 |bibcode=1976JPhA....9.1387K }}</ref>
In less formal terms, they are hypothetical long, thin defects in the fabric of space. They might have formed in the early universe during a process where certain [[symmetry breaking|symmetries were broken]]. Their existence was first contemplated by the theoretical physicist [[Tom Kibble]] in the 1970s.<ref name="Kibble 1976">{{cite journal |doi=10.1088/0305-4470/9/8/029 |title=Topology of cosmic domains and strings |year=1976 |last1=Kibble |first1=Tom W K |journal= Journal of Physics A: Mathematical and General |volume=9 |issue=8 |pages=1387–1398 |bibcode=1976JPhA....9.1387K }}</ref>
 
The formation of cosmic strings is somewhat analogous to the imperfections that form between crystal grains in solidifying liquids, or the cracks that form when water freezes into ice. The phase transitions leading to the production of cosmic strings are likely to have occurred during the earliest moments of the universe's evolution, just after [[cosmological inflation]], and are a fairly generic prediction in both [[quantum field theory]] and [[string theory]] models of the [[early universe]].
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==Dimensions==
Cosmic strings, if they exist, would be extremely thin [[topological defect]]s with diameters of the same order of magnitude as that of a proton, i.e. {{nobreak|~ 1 fm}}, or smaller. Given that this scale is much smaller than any cosmological scale, these strings are often studied in the zero-width, or Nambu–Goto approximation. Under this assumption, strings behave as one-dimensional objects and obey the [[Nambu–Goto action]], which is classically equivalent to the [[Polyakov action]] that defines the bosonic sector of [[superstring theory]].
 
In field theory, the string width is set by the scale of the symmetry -breaking [[phase transition]]. In string theory, the string width is set (in the simplest cases) by the fundamental string scale, warp factors (associated to the spacetime curvature of an internal six-dimensional spacetime manifold) and/or the size of internal [[compact dimension]]s. (In string theory, the universe is either 10- or 11-dimensional, depending on the strength of interactions and the curvature of spacetime.)
 
==Gravitation==
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===Negative mass cosmic string===
 
The [[Standard Model|standard model]] of a cosmic string is a geometrical structure with an angle deficit, which thus is in tension and hence has positive mass. In 1995, [[Matt Visser|Visser]] ''et al.'' proposed that cosmic strings could theoretically also exist with angle excesses, and thus negative tension and hence [[negative mass]]. The stability of such [[exotic matter]] strings is problematic; however, they suggested that if a negative mass string were to be wrapped around a [[wormhole]] in the early universe, such a wormhole could be stabilized sufficiently to exist in the present day.<ref>{{cite journal |arxiv=astro-ph/9409051 |bibcode=1995PhRvD..51.3117C |doi=10.1103/PhysRevD.51.3117 |pmid=10018782 |title=Natural wormholes as gravitational lenses |year=1995 |last1=Cramer |first1=John |last2=Forward |first2=Robert |last3=Morris |first3=Michael |last4=Visser |first4=Matt |last5=Benford |first5=Gregory |last6=Landis |first6=Geoffrey |journal=Physical Review D |volume=51 |issue=6 |pages=3117–3120|s2cid=42837620 }}</ref><ref>{{cite press release |url=http://www.geoffreylandis.com/wormholes.htp |title=Searching for a 'Subway to the Stars' |url-status=dead |archive-url=https://web.archive.org/web/20120415100921/http://www.geoffreylandis.com/wormholes.htp |archive-date=2012-04-15 }}</ref>
 
===Super-critical cosmic string===
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A piece of evidence supporting cosmic string theory is a phenomenon noticed in observations of the "double [[quasar]]" called [[Twin Quasar|Q0957+561A,B]]. Originally discovered by [[Dennis Walsh]], Bob Carswell, and [[Ray Weymann]] in 1979, the double image of this quasar is caused by a galaxy positioned between it and the Earth. The [[gravitational lens]] effect of this intermediate galaxy bends the quasar's light so that it follows two paths of different lengths to Earth. The result is that we see two images of the same quasar, one arriving a short time after the other (about 417.1 days later). However, a team of astronomers at the [[Harvard-Smithsonian Center for Astrophysics]] led by [[Rudolph Schild]] studied the quasar and found that during the period between September 1994 and July 1995 the two images appeared to have no time delay; changes in the brightness of the two images occurred simultaneously on four separate occasions. Schild and his team believe that the only explanation for this observation is that a cosmic string passed between the Earth and the quasar during that time period traveling at very high speed and oscillating with a period of about 100 days.<ref>{{cite journal |arxiv=astro-ph/0406434 |bibcode=2004A&A...422..477S|doi=10.1051/0004-6361:20040274 |title=Anomalous fluctuations in observations of Q0957+561 A,B: Smoking gun of a cosmic string? |year=2004 |last1=Schild |first1=R. |last2=Masnyak |first2=I. S. |last3=Hnatyk |first3=B. I. |last4=Zhdanov |first4=V. I. |journal=Astronomy and Astrophysics |volume=422 |issue=2 |pages=477–482|s2cid=16939392}}</ref>
 
CurrentlyUntil 2023 the most sensitive bounds on cosmic string parameters comecame from the non-detection of gravitational waves by [[pulsar timing array]] data.<ref>{{Cite journal|arxiv=1508.03024 |title=The NANOGrav Nine-year Data Set: Limits on the Isotropic Stochastic Gravitational Wave Background |journal=The Astrophysical Journal |volume=821 |issue=1 |pages=13 |year=2015|last1=Arzoumanian |first1=Zaven |last2=Brazier |first2=Adam |last3=Burke-Spolaor |first3=Sarah |last4=Chamberlin |first4=Sydney |last5=Chatterjee |first5=Shami |last6=Christy |first6=Brian |last7=Cordes |first7=Jim |last8=Cornish |first8=Neil |last9=Demorest |first9=Paul |last10=Deng |first10=Xihao |last11=Dolch |first11=Tim |last12=Ellis |first12=Justin |last13=Ferdman |first13=Rob |last14=Fonseca |first14=Emmanuel |last15=Garver-Daniels |first15=Nate |last16=Jenet |first16=Fredrick |last17=Jones |first17=Glenn |last18=Kaspi |first18=Vicky |last19=Koop |first19=Michael |last20=Lam |first20=Michael |last21=Lazio |first21=Joseph |last22=Levin |first22=Lina |last23=Lommen |first23=Andrea |last24=Lorimer |first24=Duncan |last25=Luo |first25=Jin |last26=Lynch |first26=Ryan |last27=Madison |first27=Dustin |last28=McLaughlin |first28=Maura |last29=McWilliams |first29=Sean |last30=Mingarelli |first30=Chiara |display-authors=29 |doi=10.3847/0004-637X/821/1/13 |bibcode = 2016ApJ...821...13A |s2cid=34191834 |doi-access=free }}</ref> The first detection of gravitational waves with pulsar timing array was confirmed in 2023.<ref>{{Cite web |last=Shelton |first=Jim |date=2023-06-28 |title=Astrophysicists present first evidence of gravitational wave ‘background’ {{!}} Yale News |url=https://news.yale.edu/2023/06/28/astrophysicists-present-first-evidence-gravitational-wave-background |access-date=2025-01-23 |website=news.yale.edu |language=en}}</ref><ref>{{Cite journal |last=Rini |first=Matteo |date=2023-06-29 |title=Researchers Capture Gravitational-Wave Background with Pulsar “Antennae” |url=https://physics.aps.org/articles/v16/118 |journal=Physics |language=en |volume=16 |pages=118}}</ref> The earthbound [[LIGO|Laser Interferometer Gravitational-Wave Observatory]] (LIGO) and especially the space-based gravitational wave detector [[Laser Interferometer Space Antenna]] (LISA) will search for gravitational waves and are likely to be sensitive enough to detect signals from cosmic strings, provided the relevant cosmic string tensions are not too small.
 
==String theory and cosmic strings==
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Much has changed since these early days, primarily due to the [[second superstring revolution]]. It is now known that string theory contains, in addition to the fundamental strings which define the theory perturbatively, other one-dimensional objects, such as D-strings, and higher-dimensional objects such as D-branes, NS-branes and M-branes partially wrapped on compact internal spacetime dimensions, while being spatially extended in one non-compact dimension. The possibility of [[Large extra dimension|large compact dimensions]] and large [[Randall–Sundrum model|warp factors]] allows strings with tension much lower than the Planck scale.
 
Furthermore, various dualities that have been discovered point to the conclusion that actually all these apparently different types of string are just the same object as it appears in different regions of [[parameter space]]. These new developments have largely revived interest in cosmic strings, starting in the early 2000s.
 
In 2002, [[Henry Tye]] and collaborators predicted the production of cosmic superstrings during the last stages of [[brane cosmology|brane inflation]],<ref>{{cite journal |arxiv=hep-th/0204074 |bibcode=2002PhLB..536..185S |doi=10.1016/S0370-2693(02)01824-5 |title=Cosmic string production towards the end of brane inflation |year=2002 |last1=Sarangi |first1=Saswat |last2=Tye |first2=S.-H.Henry |journal=Physics Letters B |volume=536 |issue=3–4 |pages=185|s2cid=14274241 }}</ref> a string theory construction of the early universe that gives leads to an expanding universe and cosmological inflation. It was subsequently realized by string theorist [[Joseph Polchinski]] that the expanding Universe could have stretched a "fundamental" string (the sort which superstring theory considers) until it was of intergalactic size. Such a stretched string would exhibit many of the properties of the old "cosmic" string variety, making the older calculations useful again. As theorist [[Tom Kibble]] remarks, "string theory cosmologists have discovered cosmic strings lurking everywhere in the undergrowth". Older proposals for detecting cosmic strings could now be used to investigate superstring theory.
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* [http://xstructure.inr.ac.ru/x-bin/theme3.py?level=1&index1=443810 Cosmic strings and superstrings on arxiv.org]
 
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