| • • • We do not use the following data for averages, fits, limits, etc. • • • |
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CMS |
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RVUE |
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3 |
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ATLS |
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4 |
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CMS |
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5 |
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ATLS |
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6 |
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CMS |
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7 |
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ATLS |
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8 |
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CMS |
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9 |
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ATLS |
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10 |
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ATLS |
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11 |
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ATLS |
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12 |
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CDF |
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1
HAYRAPETYAN 2025AK search for a new particle with lepton-flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV in the mass range 110 $<$ ${\mathit M}_{{{\mathit Z}^{\,'}}}$ $<$ 500 GeV. See their Fig. 15 for limits on $\sigma \cdot{}B$.
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CABARCAS 2024 use constraints on the non-standard neutrino interactions reported by ANTARES and IceCube expreriments to constrain ${{\mathit Z}^{\,'}}$ models with ${{\mathit \mu}}{{\mathit \tau}}$ coupling. See their Figs. 1 and 2 for limits in mass-coupling plane.
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3
AAD 2023CB search for a new particle with lepton-flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Figs.4, 5, and 6 for limits on $\sigma \cdot{}B$.
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4
TUMASYAN 2023H search for a new particle with lepton-flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 4 for limits on $\sigma \cdot{}B$.
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AABOUD 2018CM search for a new particle with lepton-flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Figs. 4, 5, and 6 for limits on $\sigma \cdot{}\mathit B$.
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SIRUNYAN 2018AT search for a narrow resonance ${{\mathit Z}^{\,'}}$ decaying into ${{\mathit e}}{{\mathit \mu}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig.5 for limit on $\sigma \cdot{}{{\mathit B}}$ in the range of 600 GeV $<$ $\mathit M_{{{\mathit Z}^{\,'}}}$ $<$ 5000 GeV.
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AABOUD 2016P search for new particle with lepton flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Figs.2, 3, and 4 for limits on ${{\mathit \sigma}}\cdot{}{{\mathit B}}$.
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KHACHATRYAN 2016BE search for new particle ${{\mathit Z}^{\,'}}$ with lepton flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at$\sqrt {s }$ = 8 TeV in the range of 200 GeV $<$ M$_{{{\mathit Z}^{\,'}}}<$ 2000 GeV. See their Fig.4 for limits on $\sigma \cdot{}\mathit B$ and their Table 5 for bounds on various masses.
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AAD 2015O search for new particle ${{\mathit Z}^{\,'}}$ with lepton flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV in the range of 500 GeV $<$ M$_{{{\mathit Z}^{\,'}}}$ $<$ 3000 GeV. See their Fig. 2 for limits on $\sigma \mathit B$.
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AAD 2011H search for new particle ${{\mathit Z}^{\,'}}$ with lepton flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV in the range of 700 GeV $<$ M$_{{{\mathit Z}^{\,'}}}$ $<$ 1000 GeV. See their Fig. 3 for limits on $\sigma \cdot{}\mathit B$.
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AAD 2011Z search for new particle ${{\mathit Z}^{\,'}}$ with lepton flavor violating decay in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV in the range 700 GeV $<$ M$_{{{\mathit Z}^{\,'}}}$ $<$ 2000 GeV. See their Fig. 3 for limits on $\sigma \cdot{}\mathit B$.
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12
ABULENCIA 2006M search for new particle ${{\mathit Z}^{\,'}}$ with lepton flavor violating decay in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96$~$TeV in the range of 100 GeV $<$ M$_{{{\mathit Z}^{\,'}}}$ $<$ 800 GeV. See their Fig.$~$4 for limits in the mass-coupling plane.
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