Light Higgs Studies for the CLIC CDR
C. Grefe, T. Laštovička, J. Strube
Abstract
Open-access reader
C. Grefe, T. Laštovička, J. Strube
Abstract
Open-access reader
The Higgs boson is the most anticipated discovery at the LHC, which can only partially explore its true nature. Thus one of the most compelling arguments to build a future linear collider is to investigate properties of the Higgs boson, especially to test the predicted linear dependence of the branching ratios on the mass of the final state. At a 3TeV CLIC machine the Higgs boson production cross section is relatively large and allows for a precision measurement of the Higgs branching ratio to pairs of b and c quarks, and even to muons. The cross section times branching ratio of the decays $H\rightarrow b\bar{b}$, $H\rightarrow c\bar{c}$ and $H\rightarrow μ^{+}μ^{-}$ can be measured with a statistical uncertainty of approximately 0.22%, 3.2% and 15%, respectively.
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The Higgs boson is the most anticipated discovery at the LHC, which can only partially explore its true nature. Thus one of the most compelling arguments to build a future linear collider is to investigate properties of the Higgs boson, especially to test the predicted linear dependence of the branching ratios on the mass of the final state. At a 3TeV CLIC machine the Higgs boson production cross section is relatively large and allows for a precision measurement of the Higgs branching ratio to pairs of b and c quarks, and even to muons. The cross section times branching ratio of the decays $H\rightarrow b\bar{b}$, $H\rightarrow c\bar{c}$ and $H\rightarrow μ^{+}μ^{-}$ can be measured with a statistical uncertainty of approximately 0.22%, 3.2% and 15%, respectively.
Key concepts: Higgs boson, Particle physics, Physics, Branching fraction, Large Hadron Collider, Muon, Nuclear physics, Bar (unit)