5 research outputs found

    Double Higgs boson production and Higgs self-coupling extraction at CLIC

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    AbstractThe Compact Linear Collider (CLIC) is a future electron–positron collider that will allow measurements of the trilinear Higgs self-coupling in double Higgs boson events produced at its high-energy stages with collision energies from s\sqrt{s} s  = 1.4 to 3 TeV. The sensitivity to the Higgs self-coupling is driven by the measurements of the cross section and the invariant mass distribution of the Higgs-boson pair in the W-boson fusion process, e+e−→HHννˉ\text {e}^{+}\text {e}^{-}\rightarrow {\text {H}\text {H}\nu \bar{\nu }} e + e - → HH ν ν ¯ . It is enhanced by including the cross-section measurement of ZHH production at 1.4 TeV. The expected sensitivity of CLIC for Higgs pair production through W-boson fusion is studied for the decay channels bbˉbbˉ\mathrm{b}\bar{\mathrm{b}}\mathrm{b}\bar{\mathrm{b}} b b ¯ b b ¯   and bbˉWW∗\mathrm{b}\bar{\mathrm{b}}\mathrm{W}\mathrm{W}^{*} b b ¯ W W ∗   using full detector simulation including all relevant backgrounds at s\sqrt{s} s = 1.4 TeV with an integrated luminosity of L\mathcal {L} L  = 2.5 ab−1^{-1} - 1 and at s\sqrt{s} s = 3 TeV with L\mathcal {L} L  = 5 ab−1^{-1} - 1 . Combining e+e−→HHννˉ\text {e}^{+}\text {e}^{-}\rightarrow {\text {H}\text {H}\nu \bar{\nu }} e + e - → HH ν ν ¯ and ZHH  cross-section measurements at 1.4 TeV with differential measurements in e+e−→HHννˉ\text {e}^{+}\text {e}^{-}\rightarrow {\text {H}\text {H}\nu \bar{\nu }} e + e - → HH ν ν ¯ events at 3 TeV, CLIC will be able to measure the trilinear Higgs self-coupling with a relative uncertainty of −8%-8\% - 8 % and +11% +11\% + 11 % at 68% C.L., assuming the Standard Model. In addition, prospects for simultaneous constraints on the trilinear Higgs self-coupling and the Higgs-gauge coupling HHWW are derived based on the HHννˉ{\text {H}\text {H}\nu \bar{\nu }} HH ν ν ¯ measurement.</jats:p

    Double Higgs boson production and Higgs self-coupling extraction at CLIC

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    The Compact Linear Collider (CLIC) is a future electron–positron collider that will allow measurements of the trilinear Higgs self-coupling in double Higgs boson events produced at its high-energy stages with collision energies from s\sqrt{s} = 1.4 to 3 TeV. The sensitivity to the Higgs self-coupling is driven by the measurements of the cross section and the invariant mass distribution of the Higgs-boson pair in the W-boson fusion process, e+e−→HHννˉ\text {e}^{+}\text {e}^{-}\rightarrow {\text {H}\text {H}\nu \bar{\nu }}. It is enhanced by including the cross-section measurement of ZHH production at 1.4 TeV. The expected sensitivity of CLIC for Higgs pair production through W-boson fusion is studied for the decay channels bbˉbbˉ\mathrm{b}\bar{\mathrm{b}}\mathrm{b}\bar{\mathrm{b}}  and bbˉWW∗\mathrm{b}\bar{\mathrm{b}}\mathrm{W}\mathrm{W}^{*}  using full detector simulation including all relevant backgrounds at s\sqrt{s} = 1.4 TeV with an integrated luminosity of L\mathcal {L} = 2.5 ab−1^{-1} and at s\sqrt{s} = 3 TeV with L\mathcal {L} = 5 ab−1^{-1}. Combining e+e−→HHννˉ\text {e}^{+}\text {e}^{-}\rightarrow {\text {H}\text {H}\nu \bar{\nu }} and ZHH  cross-section measurements at 1.4 TeV with differential measurements in e+e−→HHννˉ\text {e}^{+}\text {e}^{-}\rightarrow {\text {H}\text {H}\nu \bar{\nu }} events at 3 TeV, CLIC will be able to measure the trilinear Higgs self-coupling with a relative uncertainty of −8%-8\% and +11% +11\% at 68% C.L., assuming the Standard Model. In addition, prospects for simultaneous constraints on the trilinear Higgs self-coupling and the Higgs-gauge coupling HHWW are derived based on the HHννˉ{\text {H}\text {H}\nu \bar{\nu }} measurement.The Compact Linear Collider (CLIC) is a future electron-positron collider that will allow measurement of the trilinear Higgs self-coupling in double Higgs boson events produced at its high-energy stages with collision energies of s\sqrt{s} = 1.5 and 3 TeV. The sensitivity to the Higgs self-coupling is driven by the measurements of the cross section and the invariant mass distribution of the Higgs-boson pair in the W-boson fusion process, e+^+e−→^-\toHHνeνˉe\nu_e \bar{\nu}_e. It is enhanced by including the cross-section measurement of ZHH production at 1.5 TeV. The expected sensitivity of CLIC for Higgs pair production through W-boson fusion is studied for the decay channels bbbb and bbWW using full detector simulation including all relevant backgrounds. With an integrated luminosity of L\mathcal{L} = 5 ab−1^{-1} at s\sqrt{s} = 3 TeV, CLIC will be able to measure the trilinear Higgs self-coupling with a relative uncertainty of −8 %-8\,\% and +11 %+11\,\% at 68 %68\,\% C.L., assuming the Standard Model

    A detector for CLIC: main parameters and performance

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    Together with the recent CLIC detector model CLICdet a new software suite was introduced for the simulation and reconstruction of events in this detector. This note gives a brief introduction to CLICdet and describes the CLIC experimental conditions at 380 GeV and 3 TeV, including beam-induced backgrounds. The simulation and reconstruction tools are introduced, and the physics performance obtained is described in terms of single particles, particles in jets, jet energy resolution and flavour tagging. The performance of the very forward electromagnetic calorimeters is also discussed

    A detector for CLIC: main parameters and performance

    No full text
    Together with the recent CLIC detector model CLICdet a new software suite was introduced for the simulation and reconstruction of events in this detector. This note gives a brief introduction to CLICdet and describes the CLIC experimental conditions at 380 GeV and 3 TeV, including beam-induced backgrounds. The simulation and reconstruction tools are introduced, and the physics performance obtained is described in terms of single particles, particles in jets, jet energy resolution and flavour tagging. The performance of the very forward electromagnetic calorimeters is also discussed
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