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CP-odd contributions to the $ZZ^\ast\gamma$, $ZZ\gamma^\ast$, and $ZZZ^\ast$ vertices induced by nondiagonal charged scalar boson couplings

机译:Cp-odd贡献给$ ZZ ^ \ ast \ gamma $,$ ZZ \ gamma ^ \ ast $,和   由非对角带电标量玻色子耦合引起的$ ZZZ ^ \ ast $顶点

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摘要

In models with extended scalar sectors with several Higgs multiplets, such asHiggs triplet models, the $Z$ gauge boson can have nondiagonal couplings tocharged Higgs bosons. In a model-independent way, we study the potentialcontributions arising from such theories to the CP-violating trilinear neutralgauge boson couplings $ZZ^*\gamma$, $ZZ\gamma^*$, and $ZZZ^*$, which areparametrized by four form factors: $h^Z_{1,2}$, $f_4^\gamma$, and $f_4^Z$,respectively. Such form factors can only be induced if there are at least twonondegenerate charged Higgs scalars and an imaginary phase in the couplingconstants. For the masses of the charged scalar bosons we consider values above300 GeV and find that the form factors can reach the following orders ofmagnitude: $|h_1^Z|\sim 10^{-5}-10^{-4}$, $|h_2^Z|\sim 10^{-7}-10^{-6}$,$|f_4^\gamma|\sim 10^{-5}-10^{-3}$ and $|f_4^Z|\sim 10^{-6}-10^{-5}$, thoughthere could be an additional suppression factor arising from the couplingconstants. We also find that the form factors decouple at high energies and arenot very sensitive to a change in the masses of the charged scalar bosons.Apart from a proportionality factor, our results for the $f_4^Z$ form factor,associated with the $ZZZ^*$ vertex, is of the same order of magnitude than thatinduced via nondiagonal neutral scalar boson couplings in the framework of atwo-Higgs doublet model.
机译:在具有多个希格斯多重峰的扩展标量扇区的模型(例如希格斯三重态模型)中,$ Z $规格玻色子可以具有非对角偶合,从而带电希格斯玻色子。以与模型无关的方式,我们研究了此类理论对违反CP的三线性中性玻色子玻色子耦合$ ZZ ^ * \ gamma $,$ ZZ \ gamma ^ * $和$ ZZZ ^ * $的潜在贡献,其参数如下四个形状因子:$ h ^ Z_ {1,2} $,$ f_4 ^ \ gamma $和$ f_4 ^ Z $。仅当在耦合常数中存在至少两个非简并带电的希格斯标量和虚相时,才能诱导此类形状因子。对于带电标量玻色子的质量,我们考虑了300 GeV以上的值,并发现形状因子可以达到以下数量级:$ | h_1 ^ Z | \ sim 10 ^ {-5} -10 ^ {-4} $,$ | h_2 ^ Z | \ sim 10 ^ {-7} -10 ^ {-6} $,$ | f_4 ^ \ gamma | \ sim 10 ^ {-5} -10 ^ {-3} $和$ | f_4 ^ Z | \ sim 10 ^ {-6} -10 ^ {-5} $,认为这里可能是由耦合常数引起的附加抑制因子。我们还发现形状因数在高能下解耦,并且对带电标量玻色子质量的变化不是很敏感。除比例因数外,我们对$ f_4 ^ Z $形状因数与$ ZZZ相关的结果^ * $顶点与在atwo-Higgs doublet模型的框架中通过非对角中性标量玻色子耦合引起的顶点具有相同的数量级。

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