Search potential of the high energy-large hadron collider for spin-1/2 excited quarks in di-jet final state
Year 2024,
, 228 - 241, 11.12.2024
Yusuf Oğuzhan Günaydın
,
Mehmet Şahin
,
Leyla Aydın
Abstract
Composite models, which suggest a possible substructure of fundamental particles, can be directly proven by the discovery of the excited quark. Higher energy and higher-luminosity particle colliders are needed to discover the composite structure predicted in the proposed models. The High Energy Large Hadron Collider (HE-LHC) has the potential to be a possible discovery machine for composite models. In this collider, with a center-of-mass energy of 27 TeV and integrated luminosity between 750 and 15000 fb\textsuperscript{-1}, we calculated the exclusion, observation, and discovery limits for the mass of spin-1/2 excited quark in the \textit{di-jet} final state, as well as the attainable compositeness scale values. In addition to these calculations, we scanned free parameters from 0.06 to 1 to determine the HE-LHC potential to reveal spin-1/2 excited quark.
Thanks
We thank Usak University, Energy, Environment and Sustainability Application and Research Center for supporting this study.
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Year 2024,
, 228 - 241, 11.12.2024
Yusuf Oğuzhan Günaydın
,
Mehmet Şahin
,
Leyla Aydın
References
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https://doi.org/10.1103/PhysRevLett.14.238.
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(1974), 275–289, https://doi.org/10.1103/PhysRevD.10.275.
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265–268, https://doi.org/10.1016/0370-2693(75)90042-8.
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from 7 TeV pp collisions at CMS, Phys. Lett. B, 704 (3) (2011), 123–142,
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https://doi.org/10.1016/j.physletb.2014.09.048.
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s = 13 TeV, Phys. Rev. Lett., 116 (7) (2016), 071801, https://doi.org/10.1103/PhysRevLett.116.071801.
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pp collisions at √s=13 TeV with the ATLAS detector, Phys. Lett. B, 754 (2016), 302–322,
://doi.org/10.1016/j.physletb.2016.01.032.
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collisions at √s =13 TeV with the ATLAS detector, JHEP, 2016 (3) (2016), 41,
https://doi.org/10.1007/jhep03(2016)041.
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data collected ar √s = 13 TeV with the ATLAS detector, Phys. Rev. D, 96 (5) (2017), 052004,
https://doi.org/10.1103/PhysRevD.96.052004.
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s = 13 TeV and constraints on dark matter and other models, Phys. Lett., B769 (2017), 520–542,
https://doi.org/10.1016/j.physletb.2017.02.012.
- Sirunyan, A. M. et al., Search for narrow and broad dijet resonances in proton-proton collisions at √
s = 13 TeV and constraints on dark matter mediators and other new particles,
JHEP, 2018 (8) (2018), 130, https://doi.org/10.1007/jhep08(2018)130.
- Sirunyan, A. M. et al., Search for massive resonances decaying into WW, W Z, ZZ, qZ,
and qZ with dijet final states at √s = 13 TeV, Phys. Rev. D, 97 (7) (2018), 072006,
https://doi.org/10.1103/PhysRevD.97.072006.
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https://doi.org/10.1016/0370-2693(84)90618-X.
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Phys. Lett. B, 146 (1-2) (1984), 87–94, https://doi.org/10.1016/0370-2693(84)90649-X.
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Lett. B, 158 (3) (1985), 270–275, https://doi.org/10.1016/0370-2693(85)90969-4.
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Z. Phys. C, 29 (1) (1985), 115–122, https://doi.org/10.1007/Bf01571391.
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317–334, https://doi.org/10.1016/0550-3213(90)90040-k.
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colliders. Phys. Rev. D, 42 (3) (1990), 815–824, https://doi.org/10.1103/physrevd.42.815.
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Phys. C, 57 (3) (1993), 425–449, https://doi.org/10.1007/bf01474339.
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(3) (1999), 034004, https://doi.org/10.1103/PhysRevD.60.034004.
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collider. Phys. Rev. D, 65 (7) (2002), 075003, https://doi.org/10.1103/PhysRevD.65.075003.
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+e−, ep and pp colliders, Phys. Rev. D, 70 (7) (2004), 075011, https://doi.org/10.1103/PhysRevD.70.075011.
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at the LHC. The Eur. Phys. J. C, 32 (2) (2004), 1–17, https://doi.org/10.1140/epjcd/s2003-01-005-5.
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Phys. Rev. D, 77 (3) (2008), 035002, https://doi.org/10.1103/PhysRevD.77.035002.
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Adv. High Energy Phys., 2017 (2017), 1–9, https://doi.org/10.1155/2017/4726050.
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