Working Group Report: Higgs Boson

By S. Dawson, S. Zenz, T. Han, M. Kurata, Krishna S. Kumar, K. Fujii, K. Melnikov, K. Krueger, N. Solyak, Y. Zhang and 124 more. 2013

138 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/42cb2a89c6126207e53206e7e2d5d8c4d7ec8605

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Citations in the corpus

Physics Case for the 250 GeV Stage of the International Linear Collider (2017, background): “Earlier projections for HL-LHC are summarized in [28].”
Physics at a 100 TeV pp collider: Higgs and EW symmetry breaking studies (2016, background): “mall, there are detectable universal Higgs coupling deviations of the same order due to this tree-level mixing effect. These deviations can be detected at the percent-level at future lepton colliders [188], which are the smoking gun of Twin Higgs theories. Such a deviation, if detected at lepton col”
Knocking on new physics’ door with a scalar resonance (2015, background): “t is determined as a function of the masses and tan. The mixing is largest, ’0:3, for tan= 1, which is close to the edge of future sensitivity of the high-luminosity LHC to modied Higgs couplings [30]. Neglecting loop eects due to new (supersymmetric) particles coupled to the Higgs bosons, the produ”
Electroweak precision observables and Higgs-boson signal strengths in the Standard Model and beyond: present and future (2016, methodology): “ Phase 1 Phase 2 (Luminosity upgrade) p s[GeV] 250 500 1000 250 500 100 R Ldt[ab 1] 0.25 0.5 1 1.15 1.6 2.5 R dt(107 s) 3 3 3 3 3 3 Table 18. Expected performances of the ILC machine, taken from Ref. [88] to the Zcouplings to the 10 4 level. With this statistics, the overall uncertainty for most obs”
Gravitational wave, collider and dark matter signals from a scalar singlet electroweak baryogenesis (2017, background): “4m S ; (4.2) where F(˝) = 1 4 p ˝(˝ 1) log 1 2˝ 2 p ˝(˝ 1) 1 2˝+ 2 p ˝(˝ 1) ! : (4.3) ILC can achieve a precision of 2% whereas FCC-ee/TLEP will be able probe it with 0:6% accuracy at the 95% C.L. [57]. In Fig.2, we show parts of the model parameter space that are accessible at colliders. Clearly, ”
Building and testing models with extended Higgs sectors (2017, methodology): “ four types of avor conserving Yukawa sectors. Expected sensitivity limits for signal strengths were calculated for the LHC and future colliders. The recent Snowmass report of the Higgs working group [271] also summarizes future collider expectations for the Higgs physics, including 2HDM. Several wo”