Hexaquark

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In particle physics, hexaquarks, alternatively known as sexaquarks, [1] are a large family of hypothetical particles, each particle consisting of six quarks or antiquarks of any flavours. Six constituent quarks in any of several combinations could yield a colour charge of zero; for example a hexaquark might contain either six quarks, resembling two baryons bound together (a dibaryon), or three quarks and three antiquarks. [2] Once formed, dibaryons are predicted to be fairly stable by the standards of particle physics.

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A number of experiments have been suggested to detect dibaryon decays and interactions. In the 1990s, several candidate dibaryon decays were observed but they were not confirmed. [3] [4] [5]

There is a theory that strange particles such as hyperons [6] and dibaryons [7] [8] could form in the interior of a neutron star, changing its mass–radius ratio in ways that might be detectable. Accordingly, measurements of neutron stars could set constraints on possible dibaryon properties. [9] A large fraction of the neutrons in a neutron star could turn into hyperons and merge into dibaryons during the early part of its collapse into a black hole [ citation needed ]. These dibaryons would very quickly dissolve into quark–gluon plasma during the collapse, or go into some currently unknown state of matter.

D-star hexaquark

In 2014, a potential dibaryon was detected at the Jülich Research Center at about 2380 MeV. The center claimed that the measurements confirm results from 2011, via a more replicable method. [10] [11] The particle existed for 10−23 seconds and was named d*(2380). [12] This particle is hypothesized to consist of three up and three down quarks, and has been proposed as a candidate for dark matter. [13] [14] [15]

The study found that production of stable d*(2380) hexaquarks could account for 85% of the Universe's dark matter. [16] [17]

H dibaryon

In 1977, Robert Jaffe proposed that a possibly stable H dibaryon with the quark composition udsuds could notionally result from the combination of two uds hyperons. [18] [1] [19] [20] [21] [22] [23] [24]

Others

See also

Related Research Articles

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In particle physics, a hadron is a composite subatomic particle made of two or more quarks held together by the strong interaction. They are analogous to molecules, which are held together by the electric force. Most of the mass of ordinary matter comes from two hadrons: the proton and the neutron, while most of the mass of the protons and neutrons is in turn due to the binding energy of their constituent quarks, due to the strong force.

<span class="mw-page-title-main">Omega baryon</span> Subatomic hadron particle

Omega baryons are a family of subatomic hadrons which are represented by the symbol
Ω
and are either charge neutral or have a +2, +1 or −1 elementary charge. Additionally, they contain no up or down quarks. Omega baryons containing top quarks are also not expected to be observed. This is because the Standard Model predicts the mean lifetime of top quarks to be roughly 5×10−25 s, which is about a twentieth of the timescale necessary for the strong interactions required for Hadronization, the process by which hadrons form from quarks and gluons.

The down quark is a type of elementary particle, and a major constituent of matter. The down quark is the second-lightest of all quarks, and combines with other quarks to form composite particles called hadrons. Down quarks are most commonly found in atomic nuclei, where it combines with up quarks to form protons and neutrons. The proton is made of one down quark with two up quarks, and the neutron is made up of two down quarks with one up quark. Because they are found in every single known atom, down quarks are present in all everyday matter that we interact with.

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<span class="mw-page-title-main">Tetraquark</span> Exotic meson composed of four valence quarks

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<span class="mw-page-title-main">Exotic baryon</span> Subatomic particles; baryons with atypical quark content

In particle physics, exotic baryons are a type of hadron with half-integer spin, but with a quark content different from the three quarks (qqq) present in conventional baryons. An example would be pentaquarks, consisting of four quarks and one antiquark (qqqqq̅).

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<span class="mw-page-title-main">Exotic hadron</span> Subatomic particles consisting of quarks and gluons

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References

  1. 1 2 "Oddball sexaquark particles could be immortal, if they exist at all". Live Science . 4 February 2020.
  2. Vijande, J.; Valcarce, A.; Richard, J.-M. (2011). "Stability of hexaquarks in the string limit of confinement". Physical Review D . 85 (1): 014019. arXiv: 1111.5921 . Bibcode:2012PhRvD..85a4019V. doi:10.1103/PhysRevD.85.014019. S2CID   53511291.
  3. Belz, J.; et al. (BNL-E888 Collaboration) (1996). "Search for the weak decay of an H dibaryon". Physical Review Letters . 76 (18): 3277–3280. arXiv: hep-ex/9603002 . Bibcode:1996PhRvL..76.3277B. doi:10.1103/PhysRevLett.76.3277. PMID   10060926. S2CID   15729745.
  4. Stotzer, R. W.; et al. (BNL-E888 Collaboration) (1997). "Search for H dibaryon in 3He (K, K+) Hn". Physical Review Letters . 78 (19): 3646–36490. Bibcode:1997PhRvL..78.3646S. doi:10.1103/PhysRevLett.78.3646.
  5. Alavi-Harati, A.; et al. (KTeV Collaboration) (2000). "Search for the weak decay of a lightly bound H0 dibaryon". Physical Review Letters . 84 (12): 2593–2597. arXiv: hep-ex/9910030 . Bibcode:2000PhRvL..84.2593A. doi:10.1103/PhysRevLett.84.2593. PMID   11017277. S2CID   119068614.
  6. Ambartsumyan, V. A.; Saakyan, G. S. (1960). "The Degenerate Superdense Gas of Elementary Particles". Soviet Astronomy . 37: 193. Bibcode:1960SvA.....4..187A.
  7. Krivoruchenko, M. I. (1987). "Strange, quark, and metastable neutron stars". JETP Letters . 46 (1): 3–6. Bibcode:1987ZhPmR..46....5K.
  8. Kagiyama, S.; Nakamura, A.; Omodaka, T. (1992). "Compressible bag model and dibaryon stars". Zeitschrift für Physik C . 56 (4): 557–560. Bibcode:1992ZPhyC..56..557K. doi:10.1007/BF01474728. S2CID   121769383.
  9. Faessler, A.; Buchmann, A. J.; Krivoruchenko, M. I. (1997). "Constraints to coupling constants of the ω- and σ-mesons with dibaryons". Physical Review C . 56 (3): 1576–1581. arXiv: nucl-th/9706080 . Bibcode:1997PhRvC..56.1576F. doi:10.1103/PhysRevC.56.1576. S2CID   119392781.
  10. "Forschungszentrum Jülich press release".
  11. "Massive news in the micro-world: a hexaquark particle". The Register .
  12. Adlarson, P.; et al. (2014). "Evidence for a New Resonance from Polarized Neutron-Proton Scattering". Physical Review Letters . 112 (2): 202301. arXiv: 1402.6844 . Bibcode:2014PhRvL.112t2301A. doi:10.1103/PhysRevLett.112.202301. S2CID   2280323.
  13. Bashkanov, M. (2020). "A new possibility for light-quark dark matter". Journal of Physics G . 47 (3): 03LT01. arXiv: 2001.08654 . Bibcode:2020JPhG...47cLT01B. doi:10.1088/1361-6471/ab67e8. S2CID   210861179.
  14. "Physicists Think We Might Have a New, Exciting Dark Matter Candidate". 4 March 2020.
  15. "Did this newfound particle form the universe's dark matter?". Space.com . 5 March 2020.
  16. Williams, M. (11 March 2020). "Is the "D-star Hexaquark" the Dark Matter Particle?". Universe Today .
  17. "Ask Ethan: It's Absurd To Think Dark Matter Might Be Made Of Hexaquarks, Right?". Forbes .
  18. Jaffe, R. L. (1977). "Perhaps a Stable Dihyperon?" (PDF). Physical Review Letters . 38 (5): 195–198. Bibcode:1977PhRvL..38..195J. doi:10.1103/PhysRevLett.38.195. OSTI   1446298.
  19. Farrar, G. R. (2017). "Stable Sexaquark". arXiv: 1708.08951 [hep-ph].
  20. Kolb, E. W.; Turner, M. S. (2019). "Dibaryons cannot be the dark matter". Physical Review D . 99 (6): 063519. arXiv: 1809.06003 . Bibcode:2019PhRvD..99f3519K. doi:10.1103/PhysRevD.99.063519. S2CID   86859713.
  21. Gross, C.; Polosa, A.; Strumia, A.; Urbano, A.; Xue, W. (2018). "Dark matter in the standard model?". Physical Review D. 98 (6): 063005. arXiv: 1803.10242 . Bibcode:2018PhRvD..98f3005G. doi:10.1103/PhysRevD.98.063005. S2CID   119213361.
  22. Farrar, G. R. (2003). "A Stable H-Dibaryon: Dark Matter, Candidate Within QCD?". International Journal of Theoretical Physics . 42 (6): 1211–1218. doi:10.1023/A:1025702431127. S2CID   122452089.
  23. Farrar, G. R. (4 July 2019). "Stable Sexaquark: Dark Matter predictions, constraints and lab detection" (PDF). Quy Nhon Workshop.
  24. Azizi, K.; Agaev, S. S.; Sundu, H. (2020). "The Scalar Hexaquark uuddss: a Candidate to Dark Matter?". Journal of Physics G: Nuclear and Particle Physics. 47 (9): 095001. arXiv: 1904.09913 . Bibcode:2020JPhG...47i5001A. doi:10.1088/1361-6471/ab9a0e. S2CID   127956495.
  25. Lyu, Yan; Tong, Hui; Sugiura, Takuya; Aoki, Sinya; Doi, Takumi; Hatsuda, Tetsuo; Meng, Jie; Miyamoto, Takaya (2021-08-11). "Dibaryon with Highest Charm Number near Unitarity from Lattice QCD". Physical Review Letters. 127 (7): 072003. arXiv: 2102.00181 . Bibcode:2021PhRvL.127g2003L. doi: 10.1103/PhysRevLett.127.072003 . hdl: 2433/265092 . PMID   34459647.
  26. "Exotic six-quark particle predicted by supercomputers". www.riken.jp. Retrieved 2022-01-21.