Exotic Higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the LHeC
Abstract We study the exotic decay of the 125 GeV Higgs boson (h) into a pair of light spin-0 particles ( $$\phi $$ ϕ ) which subsequently decay and result in a 4b final state. This channel is well motivated in models with an extended Higgs sector. Instead of searching at the Large Hadron Collider (...
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doaj-669a256356d24ff8b6bcf602211622952020-11-24T21:49:13ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-07-017771910.1140/epjc/s10052-017-5012-5Exotic Higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the LHeCShang Liu0Yi-Lei Tang1Chen Zhang2Shou-hua Zhu3Institute of Theoretical Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityCenter for High Energy Physics, Peking UniversityInstitute of Theoretical Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityInstitute of Theoretical Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityAbstract We study the exotic decay of the 125 GeV Higgs boson (h) into a pair of light spin-0 particles ( $$\phi $$ ϕ ) which subsequently decay and result in a 4b final state. This channel is well motivated in models with an extended Higgs sector. Instead of searching at the Large Hadron Collider (LHC) and the high luminosity LHC (HL-LHC) which are beset by large standard model (SM) backgrounds, we investigate this decay channel at the much cleaner Large Hadron Electron Collider (LHeC). With some simple selection cuts this channel becomes nearly free of background at this ep machine, in sharp contrast to the situation at the (HL-)LHC. With a parton level analysis we show that for the $$\phi $$ ϕ mass range $$[20,60]~{\text{ GeV }}$$ [ 20 , 60 ] GeV , with $$100~{\text{ fb }^{-1}}$$ 100 fb - 1 luminosity the LHeC is generally capable of constraining $$C_{4b}^2\equiv \kappa _{V}^2\times {\mathrm {Br}}(h\rightarrow \phi \phi )\times {\mathrm {Br}}^2(\phi \rightarrow b\bar{b})$$ C 4 b 2 ≡ κ V 2 × Br ( h → ϕ ϕ ) × Br 2 ( ϕ → b b ¯ ) ( $$\kappa _{V}$$ κ V denotes the $$hVV(V=W,Z)$$ h V V ( V = W , Z ) coupling strength relative to the SM value) to a few percent level ( $$95\%$$ 95 % CLs). With $$1~{\text{ ab }^{-1}}$$ 1 ab - 1 luminosity $$C_{4b}^2$$ C 4 b 2 at a few per mille level can be probed. These sensitivities are much better than the HL-LHC performance and demonstrate the important role expected to be played by the LHeC in probing exotic Higgs decay processes, in addition to the already proposed invisible Higgs decay channel.http://link.springer.com/article/10.1140/epjc/s10052-017-5012-5 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Shang Liu Yi-Lei Tang Chen Zhang Shou-hua Zhu |
spellingShingle |
Shang Liu Yi-Lei Tang Chen Zhang Shou-hua Zhu Exotic Higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the LHeC European Physical Journal C: Particles and Fields |
author_facet |
Shang Liu Yi-Lei Tang Chen Zhang Shou-hua Zhu |
author_sort |
Shang Liu |
title |
Exotic Higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the LHeC |
title_short |
Exotic Higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the LHeC |
title_full |
Exotic Higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the LHeC |
title_fullStr |
Exotic Higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the LHeC |
title_full_unstemmed |
Exotic Higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the LHeC |
title_sort |
exotic higgs decay $$h\rightarrow \phi \phi \rightarrow 4b$$ h → ϕ ϕ → 4 b at the lhec |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2017-07-01 |
description |
Abstract We study the exotic decay of the 125 GeV Higgs boson (h) into a pair of light spin-0 particles ( $$\phi $$ ϕ ) which subsequently decay and result in a 4b final state. This channel is well motivated in models with an extended Higgs sector. Instead of searching at the Large Hadron Collider (LHC) and the high luminosity LHC (HL-LHC) which are beset by large standard model (SM) backgrounds, we investigate this decay channel at the much cleaner Large Hadron Electron Collider (LHeC). With some simple selection cuts this channel becomes nearly free of background at this ep machine, in sharp contrast to the situation at the (HL-)LHC. With a parton level analysis we show that for the $$\phi $$ ϕ mass range $$[20,60]~{\text{ GeV }}$$ [ 20 , 60 ] GeV , with $$100~{\text{ fb }^{-1}}$$ 100 fb - 1 luminosity the LHeC is generally capable of constraining $$C_{4b}^2\equiv \kappa _{V}^2\times {\mathrm {Br}}(h\rightarrow \phi \phi )\times {\mathrm {Br}}^2(\phi \rightarrow b\bar{b})$$ C 4 b 2 ≡ κ V 2 × Br ( h → ϕ ϕ ) × Br 2 ( ϕ → b b ¯ ) ( $$\kappa _{V}$$ κ V denotes the $$hVV(V=W,Z)$$ h V V ( V = W , Z ) coupling strength relative to the SM value) to a few percent level ( $$95\%$$ 95 % CLs). With $$1~{\text{ ab }^{-1}}$$ 1 ab - 1 luminosity $$C_{4b}^2$$ C 4 b 2 at a few per mille level can be probed. These sensitivities are much better than the HL-LHC performance and demonstrate the important role expected to be played by the LHeC in probing exotic Higgs decay processes, in addition to the already proposed invisible Higgs decay channel. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-017-5012-5 |
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