Next-to-leading-order corrections to the Higgs strahlung process from electron–positron collisions in extended Higgs models

Abstract We present the cross section for $$e^{+}e^{-}\rightarrow hZ$$ e + e - → h Z with arbitrary sets of electron and Z boson polarizations at the full next-to-leading order in various extended Higgs models, such as the Higgs singlet model (HSM), the inert doublet model (IDM) and the two Higgs do...

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Autores principales: Masashi Aiko, Shinya Kanemura, Kentarou Mawatari
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Publicado: SpringerOpen 2021
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spelling oai:doaj.org-article:4afcbbefaff9411d943408c2737828c42021-11-14T12:13:53ZNext-to-leading-order corrections to the Higgs strahlung process from electron–positron collisions in extended Higgs models10.1140/epjc/s10052-021-09764-81434-60441434-6052https://doaj.org/article/4afcbbefaff9411d943408c2737828c42021-11-01T00:00:00Zhttps://doi.org/10.1140/epjc/s10052-021-09764-8https://doaj.org/toc/1434-6044https://doaj.org/toc/1434-6052Abstract We present the cross section for $$e^{+}e^{-}\rightarrow hZ$$ e + e - → h Z with arbitrary sets of electron and Z boson polarizations at the full next-to-leading order in various extended Higgs models, such as the Higgs singlet model (HSM), the inert doublet model (IDM) and the two Higgs doublet model (2HDM). We systematically perform complete one-loop calculations to the helicity amplitudes in the on-shell renormalization scheme, and present the full analytic results as well as numerical evaluations. The deviation $$\Delta R^{hZ}$$ Δ R hZ in the total cross section from its standard model (SM) prediction is comprehensively analyzed, and the differences among these models are discussed in details. We find that new physics effects appearing in the renormalized hZZ vertex almost govern the behavior of $$\Delta R^{hZ}$$ Δ R hZ , and it takes a negative value in most cases. The possible size of $$\Delta R^{hZ}$$ Δ R hZ reaches several percent under the theoretical and experimental bounds. We also analyze the deviation $$\Delta R^{hZ}_{XY}$$ Δ R XY hZ in the total cross section times decay branching ratios of the discovered Higgs boson by utilizing the H-COUP program. It is found that the four types of 2HDMs can be discriminated by analyzing the correlation between $$\Delta R^{hZ}_{\tau \tau }$$ Δ R τ τ hZ and $$\Delta R^{hZ}_{bb}$$ Δ R bb hZ and those between $$\Delta R^{hZ}_{\tau \tau }$$ Δ R τ τ hZ and $$\Delta R^{hZ}_{cc}$$ Δ R cc hZ . Furthermore, the HSM and the IDM can be discriminated from the 2HDMs by measuring $$\Delta R^{hZ}_{WW}$$ Δ R WW hZ . These signatures can be tested by precision measurements at future Higgs factories such as the International Linear Collider.Masashi AikoShinya KanemuraKentarou MawatariSpringerOpenarticleAstrophysicsQB460-466Nuclear and particle physics. Atomic energy. RadioactivityQC770-798ENEuropean Physical Journal C: Particles and Fields, Vol 81, Iss 11, Pp 1-27 (2021)
institution DOAJ
collection DOAJ
language EN
topic Astrophysics
QB460-466
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
spellingShingle Astrophysics
QB460-466
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
Masashi Aiko
Shinya Kanemura
Kentarou Mawatari
Next-to-leading-order corrections to the Higgs strahlung process from electron–positron collisions in extended Higgs models
description Abstract We present the cross section for $$e^{+}e^{-}\rightarrow hZ$$ e + e - → h Z with arbitrary sets of electron and Z boson polarizations at the full next-to-leading order in various extended Higgs models, such as the Higgs singlet model (HSM), the inert doublet model (IDM) and the two Higgs doublet model (2HDM). We systematically perform complete one-loop calculations to the helicity amplitudes in the on-shell renormalization scheme, and present the full analytic results as well as numerical evaluations. The deviation $$\Delta R^{hZ}$$ Δ R hZ in the total cross section from its standard model (SM) prediction is comprehensively analyzed, and the differences among these models are discussed in details. We find that new physics effects appearing in the renormalized hZZ vertex almost govern the behavior of $$\Delta R^{hZ}$$ Δ R hZ , and it takes a negative value in most cases. The possible size of $$\Delta R^{hZ}$$ Δ R hZ reaches several percent under the theoretical and experimental bounds. We also analyze the deviation $$\Delta R^{hZ}_{XY}$$ Δ R XY hZ in the total cross section times decay branching ratios of the discovered Higgs boson by utilizing the H-COUP program. It is found that the four types of 2HDMs can be discriminated by analyzing the correlation between $$\Delta R^{hZ}_{\tau \tau }$$ Δ R τ τ hZ and $$\Delta R^{hZ}_{bb}$$ Δ R bb hZ and those between $$\Delta R^{hZ}_{\tau \tau }$$ Δ R τ τ hZ and $$\Delta R^{hZ}_{cc}$$ Δ R cc hZ . Furthermore, the HSM and the IDM can be discriminated from the 2HDMs by measuring $$\Delta R^{hZ}_{WW}$$ Δ R WW hZ . These signatures can be tested by precision measurements at future Higgs factories such as the International Linear Collider.
format article
author Masashi Aiko
Shinya Kanemura
Kentarou Mawatari
author_facet Masashi Aiko
Shinya Kanemura
Kentarou Mawatari
author_sort Masashi Aiko
title Next-to-leading-order corrections to the Higgs strahlung process from electron–positron collisions in extended Higgs models
title_short Next-to-leading-order corrections to the Higgs strahlung process from electron–positron collisions in extended Higgs models
title_full Next-to-leading-order corrections to the Higgs strahlung process from electron–positron collisions in extended Higgs models
title_fullStr Next-to-leading-order corrections to the Higgs strahlung process from electron–positron collisions in extended Higgs models
title_full_unstemmed Next-to-leading-order corrections to the Higgs strahlung process from electron–positron collisions in extended Higgs models
title_sort next-to-leading-order corrections to the higgs strahlung process from electron–positron collisions in extended higgs models
publisher SpringerOpen
publishDate 2021
url https://doaj.org/article/4afcbbefaff9411d943408c2737828c4
work_keys_str_mv AT masashiaiko nexttoleadingordercorrectionstothehiggsstrahlungprocessfromelectronpositroncollisionsinextendedhiggsmodels
AT shinyakanemura nexttoleadingordercorrectionstothehiggsstrahlungprocessfromelectronpositroncollisionsinextendedhiggsmodels
AT kentaroumawatari nexttoleadingordercorrectionstothehiggsstrahlungprocessfromelectronpositroncollisionsinextendedhiggsmodels
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