Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider

In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Majid Hashemi [verfasserIn] Gholamhossein Haghighat [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2017

Schlagwörter:	2HDM Higgs Boson Linear Collider

Übergeordnetes Werk:	In: Physics Letters B - Elsevier, 2015, 772(2017), C, Seite 426-434
Übergeordnetes Werk:	volume:772 ; year:2017 ; number:C ; pages:426-434

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc Journal toc

DOI / URN:	10.1016/j.physletb.2017.06.068

Katalog-ID:	DOAJ00307403X

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allfields	10.1016/j.physletb.2017.06.068 doi (DE-627)DOAJ00307403X (DE-599)DOAJbc8511917f3446daa422404476efb97d DE-627 ger DE-627 rakwb eng QC1-999 Majid Hashemi verfasserin aut Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. The corresponding signal significances exceed 5σ at integrated luminosity of 3000 fb−1. 2HDM Higgs Boson Linear Collider Physics Gholamhossein Haghighat verfasserin aut In Physics Letters B Elsevier, 2015 772(2017), C, Seite 426-434 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:772 year:2017 number:C pages:426-434 https://doi.org/10.1016/j.physletb.2017.06.068 kostenfrei https://doaj.org/article/bc8511917f3446daa422404476efb97d kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269317305440 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei https://doaj.org/toc/1873-2445 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 772 2017 C 426-434
spelling	10.1016/j.physletb.2017.06.068 doi (DE-627)DOAJ00307403X (DE-599)DOAJbc8511917f3446daa422404476efb97d DE-627 ger DE-627 rakwb eng QC1-999 Majid Hashemi verfasserin aut Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. The corresponding signal significances exceed 5σ at integrated luminosity of 3000 fb−1. 2HDM Higgs Boson Linear Collider Physics Gholamhossein Haghighat verfasserin aut In Physics Letters B Elsevier, 2015 772(2017), C, Seite 426-434 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:772 year:2017 number:C pages:426-434 https://doi.org/10.1016/j.physletb.2017.06.068 kostenfrei https://doaj.org/article/bc8511917f3446daa422404476efb97d kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269317305440 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei https://doaj.org/toc/1873-2445 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 772 2017 C 426-434
allfields_unstemmed	10.1016/j.physletb.2017.06.068 doi (DE-627)DOAJ00307403X (DE-599)DOAJbc8511917f3446daa422404476efb97d DE-627 ger DE-627 rakwb eng QC1-999 Majid Hashemi verfasserin aut Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. The corresponding signal significances exceed 5σ at integrated luminosity of 3000 fb−1. 2HDM Higgs Boson Linear Collider Physics Gholamhossein Haghighat verfasserin aut In Physics Letters B Elsevier, 2015 772(2017), C, Seite 426-434 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:772 year:2017 number:C pages:426-434 https://doi.org/10.1016/j.physletb.2017.06.068 kostenfrei https://doaj.org/article/bc8511917f3446daa422404476efb97d kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269317305440 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei https://doaj.org/toc/1873-2445 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 772 2017 C 426-434
allfieldsGer	10.1016/j.physletb.2017.06.068 doi (DE-627)DOAJ00307403X (DE-599)DOAJbc8511917f3446daa422404476efb97d DE-627 ger DE-627 rakwb eng QC1-999 Majid Hashemi verfasserin aut Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. The corresponding signal significances exceed 5σ at integrated luminosity of 3000 fb−1. 2HDM Higgs Boson Linear Collider Physics Gholamhossein Haghighat verfasserin aut In Physics Letters B Elsevier, 2015 772(2017), C, Seite 426-434 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:772 year:2017 number:C pages:426-434 https://doi.org/10.1016/j.physletb.2017.06.068 kostenfrei https://doaj.org/article/bc8511917f3446daa422404476efb97d kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269317305440 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei https://doaj.org/toc/1873-2445 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 772 2017 C 426-434
allfieldsSound	10.1016/j.physletb.2017.06.068 doi (DE-627)DOAJ00307403X (DE-599)DOAJbc8511917f3446daa422404476efb97d DE-627 ger DE-627 rakwb eng QC1-999 Majid Hashemi verfasserin aut Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. The corresponding signal significances exceed 5σ at integrated luminosity of 3000 fb−1. 2HDM Higgs Boson Linear Collider Physics Gholamhossein Haghighat verfasserin aut In Physics Letters B Elsevier, 2015 772(2017), C, Seite 426-434 (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:772 year:2017 number:C pages:426-434 https://doi.org/10.1016/j.physletb.2017.06.068 kostenfrei https://doaj.org/article/bc8511917f3446daa422404476efb97d kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269317305440 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei https://doaj.org/toc/1873-2445 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 772 2017 C 426-434
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title	Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider
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title_auth	Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider
abstract	In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. The corresponding signal significances exceed 5σ at integrated luminosity of 3000 fb−1.
abstractGer	In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. The corresponding signal significances exceed 5σ at integrated luminosity of 3000 fb−1.
abstract_unstemmed	In this paper, the production process e−e+→AH is analyzed in the context of the lepton-specific (or type Image 1) 2HDM and the question of observability of a neutral CP-even Higgs boson H at a linear collider operating at s=1 TeV is addressed. The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. The corresponding signal significances exceed 5σ at integrated luminosity of 3000 fb−1.
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title_short	Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider
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The CP-odd Higgs is assumed to experience a gauge-Higgs decay as A→ZH with hadronic decay of Z boson as the signature of signal events. The production chain is thus e+e−→AH→ZHH→jjℓℓℓℓ where ℓ is a τ or μ. Four benchmark points with different mass hypotheses are assumed for the analysis. The Higgs mass mH is assumed to vary within the range 150–300 GeV in increments of 50 GeV. The anti-kt algorithm is used to perform the jet reconstruction. Results indicate that the neutral CP-even Higgs H is observable through this production mechanism using the di-muon invariant mass distribution with possibility of mass measurement. 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Search for heavy neutral CP-even Higgs within lepton-specific 2HDM at a future linear collider

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