We study the sensitivity of anomalous neutral triple gauge couplings (aNTGC) via $$pp \rightarrow ZZ$$ production in the 4$$\ell $$ channel at 100 TeV center of mass energy of future circular hadron collider, FCC-hh. The analysis including the realistic detector effects is performed in the mode where both Z bosons decay into same-flavor, oppositely charged lepton pairs. The sensitivities to the charge–parity (CP)-conserving couplings $$C_{{\tilde{B}}W} / \Lambda ^{4}$$ and CP-violating couplings $$C_{WW} / \Lambda ^{4}$$ , $$C_{BW} / \Lambda ^{4}$$ and $$C_{BB} / \Lambda ^{4}$$ obtained at 95% Confidence Level using the invariant mass distribution of the 4$$\ell $$ system reconstructing the leading and sub-leading Z boson candidates are $$[-\,0.09, \,\, +\,0.09]$$ , $$[-\,0.21, \,\, +\,0.21]$$ , $$[-\,0.26, \,\, +\,0.26]$$ , and $$[-\,0.10, \,\, +\,0.10]$$ in units of $$\hbox {TeV}^{-4}$$ , respectively.
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"surname": "Denizli",
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"surname": "Turk Cakir",
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"value": "We study the sensitivity of anomalous neutral triple gauge couplings (aNTGC) via $$pp \\rightarrow ZZ$$ <math><mrow><mi>p</mi><mi>p</mi><mo>\u2192</mo><mi>Z</mi><mi>Z</mi></mrow></math> production in the 4$$\\ell $$ <math><mi>\u2113</mi></math> channel at 100 TeV center of mass energy of future circular hadron collider, FCC-hh. The analysis including the realistic detector effects is performed in the mode where both Z bosons decay into same-flavor, oppositely charged lepton pairs. The sensitivities to the charge\u2013parity (CP)-conserving couplings $$C_{{\\tilde{B}}W} / \\Lambda ^{4}$$ <math><mrow><msub><mi>C</mi><mrow><mover><mi>B</mi><mo>~</mo></mover><mi>W</mi></mrow></msub><mo>/</mo><msup><mi>\u039b</mi><mn>4</mn></msup></mrow></math> and CP-violating couplings $$C_{WW} / \\Lambda ^{4}$$ <math><mrow><msub><mi>C</mi><mrow><mi>WW</mi></mrow></msub><mo>/</mo><msup><mi>\u039b</mi><mn>4</mn></msup></mrow></math> , $$C_{BW} / \\Lambda ^{4}$$ <math><mrow><msub><mi>C</mi><mrow><mi>BW</mi></mrow></msub><mo>/</mo><msup><mi>\u039b</mi><mn>4</mn></msup></mrow></math> and $$C_{BB} / \\Lambda ^{4}$$ <math><mrow><msub><mi>C</mi><mrow><mi>BB</mi></mrow></msub><mo>/</mo><msup><mi>\u039b</mi><mn>4</mn></msup></mrow></math> obtained at 95% Confidence Level using the invariant mass distribution of the 4$$\\ell $$ <math><mi>\u2113</mi></math> system reconstructing the leading and sub-leading Z boson candidates are $$[-\\,0.09, \\,\\, +\\,0.09]$$ <math><mrow><mo>[</mo><mo>-</mo><mspace width=\"0.166667em\"></mspace><mn>0.09</mn><mo>,</mo><mspace width=\"0.166667em\"></mspace><mspace width=\"0.166667em\"></mspace><mo>+</mo><mspace width=\"0.166667em\"></mspace><mn>0.09</mn><mo>]</mo></mrow></math> , $$[-\\,0.21, \\,\\, +\\,0.21]$$ <math><mrow><mo>[</mo><mo>-</mo><mspace width=\"0.166667em\"></mspace><mn>0.21</mn><mo>,</mo><mspace width=\"0.166667em\"></mspace><mspace width=\"0.166667em\"></mspace><mo>+</mo><mspace width=\"0.166667em\"></mspace><mn>0.21</mn><mo>]</mo></mrow></math> , $$[-\\,0.26, \\,\\, +\\,0.26]$$ <math><mrow><mo>[</mo><mo>-</mo><mspace width=\"0.166667em\"></mspace><mn>0.26</mn><mo>,</mo><mspace width=\"0.166667em\"></mspace><mspace width=\"0.166667em\"></mspace><mo>+</mo><mspace width=\"0.166667em\"></mspace><mn>0.26</mn><mo>]</mo></mrow></math> , and $$[-\\,0.10, \\,\\, +\\,0.10]$$ <math><mrow><mo>[</mo><mo>-</mo><mspace width=\"0.166667em\"></mspace><mn>0.10</mn><mo>,</mo><mspace width=\"0.166667em\"></mspace><mspace width=\"0.166667em\"></mspace><mo>+</mo><mspace width=\"0.166667em\"></mspace><mn>0.10</mn><mo>]</mo></mrow></math> in units of $$\\hbox {TeV}^{-4}$$ <math><msup><mtext>TeV</mtext><mrow><mo>-</mo><mn>4</mn></mrow></msup></math> , respectively."
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