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Observation and measurement of Higgs boson decays to WW∗ with the ATLAS detector

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Observation and measurement of Higgs boson decays to WW∗ with the ATLAS detector. / The ATLAS collaboration.
In: Physical Review D, Vol. 92, No. 1, 012006, 01.07.2015.

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The ATLAS collaboration. Observation and measurement of Higgs boson decays to WW∗ with the ATLAS detector. Physical Review D. 2015 Jul 1;92(1):012006. doi: 10.1103/PhysRevD.92.012006

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The ATLAS collaboration. / Observation and measurement of Higgs boson decays to WW∗ with the ATLAS detector. In: Physical Review D. 2015 ; Vol. 92, No. 1.

Bibtex

@article{4f284cde61d64b0eb6501a6927d8be60,
title = "Observation and measurement of Higgs boson decays to WW∗ with the ATLAS detector",
abstract = "We report the observation of Higgs boson decays to WW ∗ based on an excess over background of 6.1 standard deviations in the dilepton final state, where the Standard Model expectation is 5.8 standard deviations. Evidence for the vector-boson fusion (VBF) production process is obtained with a significance of 3.2 standard deviations. The results are obtained from a data sample corresponding to an integrated luminosity of 25  fb −1 from s √ =7 and 8 TeV pp collisions recorded by the ATLAS detector at the LHC. For a Higgs boson mass of 125.36 GeV, the ratio of the measured value to the expected value of the total production cross section times branching fraction is 1.09 +0.16 −0.15 (stat) +0.17 −0.14 (syst) . The corresponding ratios for the gluon fusion and vector-boson fusion production mechanisms are 1.02±0.19(stat) +0.22 −0.18 (syst) and 1.27 +0.44 −0.40 (stat) +0.30 −0.21 (syst) , respectively. At s √ =8  TeV , the total production cross sections are measured to be σ(gg→H→WW ∗ )=4.6±0.9(stat) +0.8 −0.7 (syst)  pb and σ(VBF  H→WW ∗ )=0.51 +0.17 −0.15 (stat) +0.13 −0.08 (syst)  pb . The fiducial cross section is determined for the gluon-fusion process in exclusive final states with zero or one associated jet.",
author = "Lee Allison and Adam Barton and Michael Beattie and Guennadi Borissov and Eva Bouhova-Thacker and Alexandre Chilingarov and William Dearnaley and Harald Fox and Kathryn Grimm and Robert Henderson and Gareth Hughes and Jones, {Roger William Lewis} and Vakhtang Kartvelishvili and Robin Long and Peter Love and Harvey Maddocks and Maria Smizanska and James Walder and {The ATLAS collaboration}",
note = "This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article{\textquoteright}s title, journal citation, and DOI. {\textcopyright} 2015 CERN, for the ATLAS Collaboration ",
year = "2015",
month = jul,
day = "1",
doi = "10.1103/PhysRevD.92.012006",
language = "English",
volume = "92",
journal = "Physical Review D",
issn = "1550-7998",
publisher = "American Physical Society",
number = "1",

}

RIS

TY - JOUR

T1 - Observation and measurement of Higgs boson decays to WW∗ with the ATLAS detector

AU - Allison, Lee

AU - Barton, Adam

AU - Beattie, Michael

AU - Borissov, Guennadi

AU - Bouhova-Thacker, Eva

AU - Chilingarov, Alexandre

AU - Dearnaley, William

AU - Fox, Harald

AU - Grimm, Kathryn

AU - Henderson, Robert

AU - Hughes, Gareth

AU - Jones, Roger William Lewis

AU - Kartvelishvili, Vakhtang

AU - Long, Robin

AU - Love, Peter

AU - Maddocks, Harvey

AU - Smizanska, Maria

AU - Walder, James

AU - The ATLAS collaboration

N1 - This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. © 2015 CERN, for the ATLAS Collaboration

PY - 2015/7/1

Y1 - 2015/7/1

N2 - We report the observation of Higgs boson decays to WW ∗ based on an excess over background of 6.1 standard deviations in the dilepton final state, where the Standard Model expectation is 5.8 standard deviations. Evidence for the vector-boson fusion (VBF) production process is obtained with a significance of 3.2 standard deviations. The results are obtained from a data sample corresponding to an integrated luminosity of 25  fb −1 from s √ =7 and 8 TeV pp collisions recorded by the ATLAS detector at the LHC. For a Higgs boson mass of 125.36 GeV, the ratio of the measured value to the expected value of the total production cross section times branching fraction is 1.09 +0.16 −0.15 (stat) +0.17 −0.14 (syst) . The corresponding ratios for the gluon fusion and vector-boson fusion production mechanisms are 1.02±0.19(stat) +0.22 −0.18 (syst) and 1.27 +0.44 −0.40 (stat) +0.30 −0.21 (syst) , respectively. At s √ =8  TeV , the total production cross sections are measured to be σ(gg→H→WW ∗ )=4.6±0.9(stat) +0.8 −0.7 (syst)  pb and σ(VBF  H→WW ∗ )=0.51 +0.17 −0.15 (stat) +0.13 −0.08 (syst)  pb . The fiducial cross section is determined for the gluon-fusion process in exclusive final states with zero or one associated jet.

AB - We report the observation of Higgs boson decays to WW ∗ based on an excess over background of 6.1 standard deviations in the dilepton final state, where the Standard Model expectation is 5.8 standard deviations. Evidence for the vector-boson fusion (VBF) production process is obtained with a significance of 3.2 standard deviations. The results are obtained from a data sample corresponding to an integrated luminosity of 25  fb −1 from s √ =7 and 8 TeV pp collisions recorded by the ATLAS detector at the LHC. For a Higgs boson mass of 125.36 GeV, the ratio of the measured value to the expected value of the total production cross section times branching fraction is 1.09 +0.16 −0.15 (stat) +0.17 −0.14 (syst) . The corresponding ratios for the gluon fusion and vector-boson fusion production mechanisms are 1.02±0.19(stat) +0.22 −0.18 (syst) and 1.27 +0.44 −0.40 (stat) +0.30 −0.21 (syst) , respectively. At s √ =8  TeV , the total production cross sections are measured to be σ(gg→H→WW ∗ )=4.6±0.9(stat) +0.8 −0.7 (syst)  pb and σ(VBF  H→WW ∗ )=0.51 +0.17 −0.15 (stat) +0.13 −0.08 (syst)  pb . The fiducial cross section is determined for the gluon-fusion process in exclusive final states with zero or one associated jet.

U2 - 10.1103/PhysRevD.92.012006

DO - 10.1103/PhysRevD.92.012006

M3 - Journal article

VL - 92

JO - Physical Review D

JF - Physical Review D

SN - 1550-7998

IS - 1

M1 - 012006

ER -