We ask for explanations for
- unification of Standard Model and general relativity,
- dark matter and dark energy,
- large matter antimatter asymmetry,
- cosmic inflation,
- …
Can the Higgs boson provide a glimpse on, or direction to these problems?
04/26/16
We ask for explanations for
Can the Higgs boson provide a glimpse on, or direction to these problems?
(CMS-HIG-14-009)
Higgs boson is an essential (residual) particle from EWSB in the SM. It unitarizes longitudinal WW boson scattering. Its mass, as a scalar particle, is sensitive to UV physics.
Is the SM Higgs boson solely responsible for EWSB?
Parametrize Higgs-gluon coupling by dim.-7 operators (Gracey '02; Neill '09; Germer '07)
\[\begin{multline*} \mathcal{L}_{eff}=\frac{\color{black}{C_{1}}}{\color{red}{\Lambda}}HF_{\mu\nu}^{a}F^{a\,\mu\nu} +\frac{\color{black}{C_{2}}}{\color{red}{\Lambda^{3}}}HD_{\alpha}F_{\mu\nu}^{a}D^{\alpha}F^{a\,\mu\nu}+\frac{\color{black}{C_{3}}}{\color{red}{\Lambda^{3}}}HF_{\nu}^{a\,\mu}F_{\sigma}^{b\,\nu}F_{\mu}^{c\,\sigma}f^{abc}\\ +\frac{\color{black}{C_{4}}}{\color{red}{\Lambda^{3}}}HD^{\alpha}F_{\alpha\nu}^{a}D_{\beta}F^{a\,\beta\nu}+\frac{\color{black}{C_{5}}}{\color{red}{\Lambda^{3}}}HF_{\alpha\nu}^{a}D^{\nu}D^{\beta}F_{\beta}^{a\,\alpha} \\ \equiv \frac{\color{black}{C_{1}}}{\color{red}{\Lambda}} \mathcal{O}_1 + \frac{\color{black}{C_{2}}}{\color{red}{\Lambda^3}} \mathcal{O}_2 + \frac{\color{black}{C_{3}}}{\color{red}{\Lambda^3}} \mathcal{O}_3 + \frac{\color{black}{C_{4}}}{\color{red}{\Lambda^3}} \mathcal{O}_4 + \frac{\color{black}{C_{5}}}{\color{red}{\Lambda^3}} \mathcal{O}_5 \end{multline*} \]
Normalization to corresponding part of cross-section: only shape matters here; coefficients \(C_i\) a priori unknown. (Harlander, Neumann '13)
\[ F(\Gamma) \to \sum_\gamma \mathcal{T} F(\gamma) \star F(\Gamma\backslash\gamma) \]
lead to the NLO one-loop revolution: i.e. BlackHat, GoSam, HelacNLO, MadLoop, OpenLoops, Rocket, …
efficiently implemented in MCFM (POWHEG-BOX soon)
(Neumann, Williams 1605.XXXXX)