The effective field theory for single Higgs and double Higgs production beyond leading order
Authors
Long-Bin Chen
- Guangzhou University
- chenlb_AT_gzhu_dot_edu_dot_cn
Hai Tao Li
- LANL
- haitaoli_AT_lanl_dot_gov
Hua-Sheng Shao
- LPTHE
- huasheng_dot_shao_AT_lpthe_dot_jussieu_dot_fr
Jian Wang
- Shandong University
- j_dot_wang_AT_sdu_dot_edu_dot_cn
References
- L.-B. Chen, H. T. Li, H.-S. Shao and J. Wang, arXiv:1909.06808, arXiv:1912.13001.
Description of the model
In the infinite top-quark mass limit, the interaction between the Higgs field and the gluon field can be effectively described by
$\mathcal{L}_{\rm eff}=-\frac{1}{4}(C_h \frac{h}{v}-C_{hh}\frac{h^2}{2v^2})G^a_{\mu\nu}G^{a~\mu\nu}$
where $G^a_{\mu\nu}$
The NLO UFO model based on $\mathcal{L}_{\rm eff}+\mathcal{L}_{\rm SM}$
The analytical expressions for $R_2$
An example in MadGraph5_aMC@NLO
In order to handle mixed-order senarios, one has to use the version 3.0.1+ of MadGraph5_aMC@NLO.
In version 3.0.X, the NLO QCD correction to di-Higgs+jet at $\mathcal{O}(\alpha_s^3)$
> import model HEFT_DH_UFO > generate p p > h h j / t t~ QCD=3 QED=2 NP=2 [QCD] QCD^2<=6 QED^2<=4 NP^2<=4
In versions 3.1.0+, the generation syntax has been changed here. It is generated by two processes, i.e.,
> import model HEFT_DH_UFO > generate p p > h h j / t t~ QCD=3 QED=2 NP=2 [QCD] QCD^2<=6 QED^2<=4 NP^2<=4
and
> import model HEFT_DH_UFO > generate p p > h h j / t t~ QCD^2==8 QED^2<=4 NP^2<=4
The second part is the pure interference term at tree level but contributing to $\mathcal{O}(\alpha_s^4)$