We test the Electric Charged Swap (ECS) symmetry in the case of quarks. We propose a quark (q)- and an ECS-quark (q῀)-bound state, qq῀. We explain the electrically charged charmonium Z+c (3, 9) meson as a charm quark (c)- and charm ECS-quark (c῀)- nonrelativistic bound state (cc῀). We predict that J/ψ and π+ mesons are the decay products of a Z+c (3, 9), as it has been recently observed at the Beijing Electron Positron Collider (BES) III. Furthermore, from the charm ECS-quark (c῀) of mass 2,3GeV we predict two new mesons, an electrically charged charmed meson D¯*+(zm) and a neutral charmed meson D*0(zm).
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International Journal of High Energy Physics (Volume 2, Issue 4-1)
This article belongs to the Special Issue Symmetries in Relativity, Quantum Theory, and Unified Theories |
| DOI | 10.11648/j.ijhep.s.2015020401.11 |
| Page(s) | 1-7 |
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Group Theory, Exotic Mesons, Hypothetical Particles
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APA Style
E. Koorambas. (2015). Quark–Quark of Swap Electric Charge Bound State. International Journal of High Energy Physics, 2(4-1), 1-7. https://doi.org/10.11648/j.ijhep.s.2015020401.11
ACS Style
E. Koorambas. Quark–Quark of Swap Electric Charge Bound State. Int. J. High Energy Phys. 2015, 2(4-1), 1-7. doi: 10.11648/j.ijhep.s.2015020401.11
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Download@article{10.11648/j.ijhep.s.2015020401.11,
author = {E. Koorambas},
title = {Quark–Quark of Swap Electric Charge Bound State},
journal = {International Journal of High Energy Physics},
volume = {2},
number = {4-1},
pages = {1-7},
doi = {10.11648/j.ijhep.s.2015020401.11},
url = {https://doi.org/10.11648/j.ijhep.s.2015020401.11},
eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ijhep.s.2015020401.11},
abstract = {We test the Electric Charged Swap (ECS) symmetry in the case of quarks. We propose a quark (q)- and an ECS-quark (q῀)-bound state, qq῀. We explain the electrically charged charmonium Z+c (3, 9) meson as a charm quark (c)- and charm ECS-quark (c῀)- nonrelativistic bound state (cc῀). We predict that J/ψ and π+ mesons are the decay products of a Z+c (3, 9), as it has been recently observed at the Beijing Electron Positron Collider (BES) III. Furthermore, from the charm ECS-quark (c῀) of mass 2,3GeV we predict two new mesons, an electrically charged charmed meson D¯*+(zm) and a neutral charmed meson D*0(zm).},
year = {2015}
}
TY - JOUR T1 - Quark–Quark of Swap Electric Charge Bound State AU - E. Koorambas Y1 - 2015/06/09 PY - 2015 N1 - https://doi.org/10.11648/j.ijhep.s.2015020401.11 DO - 10.11648/j.ijhep.s.2015020401.11 T2 - International Journal of High Energy Physics JF - International Journal of High Energy Physics JO - International Journal of High Energy Physics SP - 1 EP - 7 PB - Science Publishing Group SN - 2376-7448 UR - https://doi.org/10.11648/j.ijhep.s.2015020401.11 AB - We test the Electric Charged Swap (ECS) symmetry in the case of quarks. We propose a quark (q)- and an ECS-quark (q῀)-bound state, qq῀. We explain the electrically charged charmonium Z+c (3, 9) meson as a charm quark (c)- and charm ECS-quark (c῀)- nonrelativistic bound state (cc῀). We predict that J/ψ and π+ mesons are the decay products of a Z+c (3, 9), as it has been recently observed at the Beijing Electron Positron Collider (BES) III. Furthermore, from the charm ECS-quark (c῀) of mass 2,3GeV we predict two new mesons, an electrically charged charmed meson D¯*+(zm) and a neutral charmed meson D*0(zm). VL - 2 IS - 4-1 ER -
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