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Vršni kvark
Događaj sudara u kome učestvuje vršni kvark
KompozicijaElementarna čestica
StatistikeFermionska
GeneracijaTreća
InterakcijeJaka, slaba, elektromagnetna sila, gravitacija
Simbolt
AntičesticaVršni antikvark (t)
TeorijeMakoto Kobajaši i Tošihide Maskava (1973)
OtkrivenCDF i DØ kolaboracije (1995)
Masa173,0 ± 0,4 GeV/c2[1]
Raspad uDubinski kvark (99,8%)
strani kvark (0,17%)
donji kvark (0,007%)
Naelektrisanje+2/3 e
Boja nabojaDa
Spin1/2
Vrh1
Slabi izospinLH: +1/2, RH: 0
Slabi hipernabojLH: +1/3, RH: +4/3

Vršni kvark (engl. top quark), takođe poznat kao t kvark (simbol: t) ili kvark istine, najmasivniji je od svih uočenih elementarnih čestica. Like all quarks, the top quark is a fermion with spin 1/2, and experiences all four fundamental interactions: gravitation, electromagnetism, weak interactions, and strong interactions. It has an electric charge of +2/3 e. It has a mass of 173.0 ± 0.4 GeV/c2,[1] which is about the same mass as an atom of rhenium.[2] The antiparticle of the top quark is the top antiquark (symbol: t, sometimes called antitop quark or simply antitop), which differs from it only in that some of its properties have equal magnitude but opposite sign.

Vršni kvark interacts primarily by the strong interaction, but can only decay through the weak force. It decays to a W boson and either a bottom quark (most frequently), a strange quark, or, on the rarest of occasions, a down quark. The Standard Model predicts its mean lifetime to be roughly 5×10−25 s.[3] This is about a twentieth of the timescale for strong interactions, and therefore it does not form hadrons, giving physicists a unique opportunity to study a "bare" quark (all other quarks hadronize, meaning that they combine with other quarks to form hadrons, and can only be observed as such). Because it is so massive, the properties of the top quark allow predictions to be made of the mass of the Higgs boson under certain extensions of the Standard Model (see Mass and coupling to the Higgs boson below). As such, it is extensively studied as a means to discriminate between competing theories.

Its existence (and that of the bottom quark) was postulated in 1973 by Makoto Kobayashi and Toshihide Maskawa to explain the observed CP violations in kaon decay,[4] and was discovered in 1995 by the CDF[5] and DØ[6] experiments at Fermilab. Kobayashi and Maskawa won the 2008 Nobel Prize in Physics for the prediction of the top and bottom quark, which together form the third generation of quarks.[7]

Istorija

In 1973, Makoto Kobayashi and Toshihide Maskawa predicted the existence of a third generation of quarks to explain observed CP violations in kaon decay.[4] The names top and bottom were introduced by Haim Harari in 1975,[8][9] to match the names of the first generation of quarks (up and down) reflecting the fact that the two were the 'up' and 'down' component of a weak isospin doublet.[10] The top quark was sometimes called truth quark in the past, but over time top quark became the predominant use.[11]

The proposal of Kobayashi and Maskawa heavily relied on the GIM mechanism put forward by Sheldon Lee Glashow, John Iliopoulos and Luciano Maiani,[12] which predicted the existence of the then still unobserved charm quark. (The other second generation quark, the strange quark, was already detected in 1968.) When in November 1974 teams at Brookhaven National Laboratory (BNL) and the Stanford Linear Accelerator Center (SLAC) simultaneously announced the discovery of the J/ψ meson, it was soon after identified as a bound state of the missing charm quark with its antiquark. This discovery allowed the GIM mechanism to become part of the Standard Model.[13] With the acceptance of the GIM mechanism, Kobayashi and Maskawa's prediction also gained in credibility. Their case was further strengthened by the discovery of the tau by Martin Lewis Perl's team at SLAC between 1974 and 1978.[14] The tau announced a third generation of leptons, breaking the new symmetry between leptons and quarks introduced by the GIM mechanism. Restoration of the symmetry implied the existence of a fifth and sixth quark.

It was in fact not long until a fifth quark, the bottom, was discovered by the E288 experiment team, led by Leon Lederman at Fermilab in 1977.[15][16][17] This strongly suggested that there must also be a sixth quark, the top, to complete the pair. It was known that this quark would be heavier than the bottom, requiring more energy to create in particle collisions, but the general expectation was that the sixth quark would soon be found. However, it took another 18 years before the existence of the top was confirmed.[18]

Early searches for the top quark at SLAC and DESY (in Hamburg) came up empty-handed. When, in the early eighties, the Super Proton Synchrotron (SPS) at CERN discovered the W boson and the Z boson, it was again felt that the discovery of the top was imminent. As the SPS gained competition from the Tevatron at Fermilab there was still no sign of the missing particle, and it was announced by the group at CERN that the top mass must be at least 41 GeV/c2. After a race between CERN and Fermilab to discover the top, the accelerator at CERN reached its limits without creating a single top, pushing the lower bound on its mass up to 77 GeV/c2.[18]

The Tevatron was (until the start of LHC operation at CERN in 2009) the only hadron collider powerful enough to produce top quarks. In order to be able to confirm a future discovery, a second detector, the DØ detector, was added to the complex (in addition to the Collider Detector at Fermilab (CDF) already present). In October 1992, the two groups found their first hint of the top, with a single creation event that appeared to contain the top. In the following years, more evidence was collected and on April 22, 1994, the CDF group submitted their paper presenting tentative evidence for the existence of a top quark with a mass of about 175 GeV/c2. In the meantime, DØ had found no more evidence than the suggestive event in 1992. A year later, on March 2, 1995, after having gathered more evidence and reanalyzed the DØ data (which had been searched for a much lighter top), the two groups jointly reported the discovery of the top at a mass of 176±18 GeV/c2.[5][6][18]

In the years leading up to the top quark discovery, it was realized that certain precision measurements of the electroweak vector boson masses and couplings are very sensitive to the value of the top quark mass. These effects become much larger for higher values of the top mass and therefore could indirectly see the top quark even if it could not be directly detected in any experiment at the time. The largest effect from the top quark mass was on the T parameter and by 1994 the precision of these indirect measurements had led to a prediction of the top quark mass to be between 145 GeV/c2 and 185 GeV/c2.[19] It is the development of techniques that ultimately allowed such precision calculations that led to Gerardus 't Hooft and Martinus Veltman winning the Nobel Prize in physics in 1999.[20][21]

Reference

  1. ^ а б M. Tanabashi et al. (Particle Data Group) (2018). „Review of Particle Physics”. Physical Review D. 98 (3): 030001. doi:10.1103/PhysRevD.98.030001. 
  2. ^ Elert, Glenn. „Quantum Chromodynamics”. The Physics Hypertextbook. Приступљено 2019-03-23. 
  3. ^ A. Quadt (2006). „Top quark physics at hadron colliders”. European Physical Journal C. 48 (3): 835—1000. Bibcode:2006EPJC...48..835Q. doi:10.1140/epjc/s2006-02631-6. 
  4. ^ а б M. Kobayashi; T. Maskawa (1973). „CP-Violation in the Renormalizable Theory of Weak Interaction”. Progress of Theoretical Physics. 49 (2): 652. Bibcode:1973PThPh..49..652K. doi:10.1143/PTP.49.652. 
  5. ^ а б F. Abe et al. (CDF Collaboration) (1995). „Observation of Top Quark Production in pp Collisions with the Collider Detector at Fermilab”. Physical Review Letters. 74 (14): 2626—2631. Bibcode:1995PhRvL..74.2626A. PMID 10057978. arXiv:hep-ex/9503002 Слободан приступ. doi:10.1103/PhysRevLett.74.2626. 
  6. ^ а б S. Abachi et al. (DØ Collaboration) (1995). „Search for High Mass Top Quark Production in pp Collisions at √s = 1.8 TeV”. Physical Review Letters. 74 (13): 2422—2426. Bibcode:1995PhRvL..74.2422A. PMID 10057924. arXiv:hep-ex/9411001 Слободан приступ. doi:10.1103/PhysRevLett.74.2422. 
  7. ^ „2008 Nobel Prize in Physics”. The Nobel Foundation. 2008. Приступљено 2009-09-11. 
  8. ^ H. Harari (1975). „A new quark model for hadrons”. Physics Letters B. 57 (3): 265. Bibcode:1975PhLB...57..265H. doi:10.1016/0370-2693(75)90072-6. 
  9. ^ K.W. Staley (2004). The Evidence for the Top Quark. Cambridge University Press. стр. 31—33. ISBN 978-0-521-82710-2. 
  10. ^ D.H. Perkins (2000). Introduction to high energy physics. Cambridge University Press. стр. 8. ISBN 978-0-521-62196-0. 
  11. ^ F. Close (2006). The New Cosmic Onion. CRC Press. стр. 133. ISBN 978-1-58488-798-0. 
  12. ^ S.L. Glashow; J. Iliopoulous; L. Maiani (1970). „Weak Interactions with Lepton–Hadron Symmetry”. Physical Review D. 2 (7): 1285—1292. Bibcode:1970PhRvD...2.1285G. doi:10.1103/PhysRevD.2.1285. 
  13. ^ A. Pickering (1999). Constructing Quarks: A Sociological History of Particle Physics. University of Chicago Press. стр. 253—254. ISBN 978-0-226-66799-7. 
  14. ^ M.L. Perl; et al. (1975). „Evidence for Anomalous Lepton Production in e+e− Annihilation”. Physical Review Letters. 35 (22): 1489. Bibcode:1975PhRvL..35.1489P. doi:10.1103/PhysRevLett.35.1489. 
  15. ^ „Discoveries at Fermilab – Discovery of the Bottom Quark” (Саопштење). Fermilab. 7. 8. 1977. Приступљено 2009-07-24. 
  16. ^ L.M. Lederman (2005). „Logbook: Bottom Quark”. Symmetry Magazine. 2 (8). Архивирано из оригинала 2006-10-04. г. 
  17. ^ S.W. Herb; et al. (1977). „Observation of a Dimuon Resonance at 9.5 GeV in 400-GeV Proton-Nucleus Collisions”. Physical Review Letters. 39 (5): 252. Bibcode:1977PhRvL..39..252H. doi:10.1103/PhysRevLett.39.252. 
  18. ^ а б в T.M. Liss; P.L. Tipton (1997). „The Discovery of the Top Quark” (PDF). Scientific American. 277 (3): 54—59. doi:10.1038/scientificamerican0997-54. 
  19. ^ The Discovery of the Top Quark, Tony M. Liss and Paul L. Tipton
  20. ^ „The Nobel Prize in Physics 1999”. The Nobel Foundation. Приступљено 2009-09-10. 
  21. ^ „The Nobel Prize in Physics 1999, Press Release” (Саопштење). The Nobel Foundation. 12. 10. 1999. Приступљено 2009-09-10. 

Literatura

Spoljašnje veze

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