MSSM Higgs searches in multi-b-jet final states at the LHC
Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 1...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Richter-Wcas, Elżbieta [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1997 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer-Verlag 1997 |
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| Übergeordnetes Werk: |
Enthalten in: Zeitschrift für Physik - Berlin : Springer, 1979, 76(1997), 4 vom: Dez., Seite 665-676 |
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| Übergeordnetes Werk: |
volume:76 ; year:1997 ; number:4 ; month:12 ; pages:665-676 |
| Links: |
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| DOI / URN: |
10.1007/s002880050589 |
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| Katalog-ID: |
SPR003729516 |
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| 100 | 1 | |a Richter-Wcas, Elżbieta |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a MSSM Higgs searches in multi-b-jet final states at the LHC |
| 264 | 1 | |c 1997 | |
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| 500 | |a © Springer-Verlag 1997 | ||
| 520 | |a Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. | ||
| 650 | 4 | |a Minimal Supersymmetric Standard Model |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Background Event |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Integrate Luminosity |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Mass Window |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Minimal Supersymmetric Standard Model Higgs Boson |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Froidevaux, Daniel |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Zeitschrift für Physik |d Berlin : Springer, 1979 |g 76(1997), 4 vom: Dez., Seite 665-676 |w (DE-627)254911307 |w (DE-600)1463347-4 |x 1431-5858 |7 nnns |
| 773 | 1 | 8 | |g volume:76 |g year:1997 |g number:4 |g month:12 |g pages:665-676 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s002880050589 |z lizenzpflichtig |3 Volltext |
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1997 |
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1997 |
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10.1007/s002880050589 doi (DE-627)SPR003729516 (SPR)s002880050589-e DE-627 ger DE-627 rakwb eng Richter-Wcas, Elżbieta verfasserin aut MSSM Higgs searches in multi-b-jet final states at the LHC 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. Minimal Supersymmetric Standard Model (dpeaa)DE-He213 Background Event (dpeaa)DE-He213 Integrate Luminosity (dpeaa)DE-He213 Mass Window (dpeaa)DE-He213 Minimal Supersymmetric Standard Model Higgs Boson (dpeaa)DE-He213 Froidevaux, Daniel aut Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 76(1997), 4 vom: Dez., Seite 665-676 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:76 year:1997 number:4 month:12 pages:665-676 https://dx.doi.org/10.1007/s002880050589 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 76 1997 4 12 665-676 |
| spelling |
10.1007/s002880050589 doi (DE-627)SPR003729516 (SPR)s002880050589-e DE-627 ger DE-627 rakwb eng Richter-Wcas, Elżbieta verfasserin aut MSSM Higgs searches in multi-b-jet final states at the LHC 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. Minimal Supersymmetric Standard Model (dpeaa)DE-He213 Background Event (dpeaa)DE-He213 Integrate Luminosity (dpeaa)DE-He213 Mass Window (dpeaa)DE-He213 Minimal Supersymmetric Standard Model Higgs Boson (dpeaa)DE-He213 Froidevaux, Daniel aut Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 76(1997), 4 vom: Dez., Seite 665-676 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:76 year:1997 number:4 month:12 pages:665-676 https://dx.doi.org/10.1007/s002880050589 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 76 1997 4 12 665-676 |
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10.1007/s002880050589 doi (DE-627)SPR003729516 (SPR)s002880050589-e DE-627 ger DE-627 rakwb eng Richter-Wcas, Elżbieta verfasserin aut MSSM Higgs searches in multi-b-jet final states at the LHC 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. Minimal Supersymmetric Standard Model (dpeaa)DE-He213 Background Event (dpeaa)DE-He213 Integrate Luminosity (dpeaa)DE-He213 Mass Window (dpeaa)DE-He213 Minimal Supersymmetric Standard Model Higgs Boson (dpeaa)DE-He213 Froidevaux, Daniel aut Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 76(1997), 4 vom: Dez., Seite 665-676 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:76 year:1997 number:4 month:12 pages:665-676 https://dx.doi.org/10.1007/s002880050589 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 76 1997 4 12 665-676 |
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10.1007/s002880050589 doi (DE-627)SPR003729516 (SPR)s002880050589-e DE-627 ger DE-627 rakwb eng Richter-Wcas, Elżbieta verfasserin aut MSSM Higgs searches in multi-b-jet final states at the LHC 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. Minimal Supersymmetric Standard Model (dpeaa)DE-He213 Background Event (dpeaa)DE-He213 Integrate Luminosity (dpeaa)DE-He213 Mass Window (dpeaa)DE-He213 Minimal Supersymmetric Standard Model Higgs Boson (dpeaa)DE-He213 Froidevaux, Daniel aut Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 76(1997), 4 vom: Dez., Seite 665-676 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:76 year:1997 number:4 month:12 pages:665-676 https://dx.doi.org/10.1007/s002880050589 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 76 1997 4 12 665-676 |
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10.1007/s002880050589 doi (DE-627)SPR003729516 (SPR)s002880050589-e DE-627 ger DE-627 rakwb eng Richter-Wcas, Elżbieta verfasserin aut MSSM Higgs searches in multi-b-jet final states at the LHC 1997 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 1997 Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. Minimal Supersymmetric Standard Model (dpeaa)DE-He213 Background Event (dpeaa)DE-He213 Integrate Luminosity (dpeaa)DE-He213 Mass Window (dpeaa)DE-He213 Minimal Supersymmetric Standard Model Higgs Boson (dpeaa)DE-He213 Froidevaux, Daniel aut Enthalten in Zeitschrift für Physik Berlin : Springer, 1979 76(1997), 4 vom: Dez., Seite 665-676 (DE-627)254911307 (DE-600)1463347-4 1431-5858 nnns volume:76 year:1997 number:4 month:12 pages:665-676 https://dx.doi.org/10.1007/s002880050589 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 76 1997 4 12 665-676 |
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Enthalten in Zeitschrift für Physik 76(1997), 4 vom: Dez., Seite 665-676 volume:76 year:1997 number:4 month:12 pages:665-676 |
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Minimal Supersymmetric Standard Model Background Event Integrate Luminosity Mass Window Minimal Supersymmetric Standard Model Higgs Boson |
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Richter-Wcas, Elżbieta @@aut@@ Froidevaux, Daniel @@aut@@ |
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Richter-Wcas, Elżbieta |
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MSSM Higgs searches in multi-b-jet final states at the LHC Minimal Supersymmetric Standard Model (dpeaa)DE-He213 Background Event (dpeaa)DE-He213 Integrate Luminosity (dpeaa)DE-He213 Mass Window (dpeaa)DE-He213 Minimal Supersymmetric Standard Model Higgs Boson (dpeaa)DE-He213 |
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MSSM Higgs searches in multi-b-jet final states at the LHC |
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mssm higgs searches in multi-b-jet final states at the lhc |
| title_auth |
MSSM Higgs searches in multi-b-jet final states at the LHC |
| abstract |
Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. © Springer-Verlag 1997 |
| abstractGer |
Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. © Springer-Verlag 1997 |
| abstract_unstemmed |
Abstract This paper discusses the possibility to observe a signal from MSSM Higgs boson decays into final states containing four b-jets. Two specific channels are considered: bb̄H and bb̄A production with H,A → bb̄, for large values of $ m_{H} $, $ m_{A} $ and tan β, and H → hh → bb̄bb̄ decays for 150 GeV < $ m_{H} $ < $ 2m_{t} $ and for low values of tan β. Both channels are difficult to extract because of the very large reducible and irreducible QCD backgrounds. Even with an ultimate integrated luminosity, expected per LHC experiment, of 3 · $ 10^{5} $ $ pb^{-1} $, the region of the MSSM parameter space covered by these channels does not extend the reach beyond that accessible to other channels that were studied in the past. Nevertheless, their observation would help in constraining the couplings and branching ratios of the MSSM Higgs bosons. © Springer-Verlag 1997 |
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| title_short |
MSSM Higgs searches in multi-b-jet final states at the LHC |
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https://dx.doi.org/10.1007/s002880050589 |
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Froidevaux, Daniel |
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10.1007/s002880050589 |
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2024-07-03T21:17:55.329Z |
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| score |
7.3999643 |