04/26/16

Standard Model can't be the complete deal…

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?

…but Higgs physics looks SM like.

(CMS-HIG-14-009)

The Standard Model Higgs?!

Higgs at high \(p_T\): outlining questions

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?

  • We need precise predictions to interpret data: test SM-only hypothesis, constrain BSM models.
    • Methods to quantify deviations
  • We should focus on the most promising kinematical regions.
    • High Higgs transverse momenta (\(p_T\))

Is the H-gluon coupling top-quark loop induced?

How do we quantify deviations from the SM?

  • modify SM couplings (rescale parameters and couplings)
  • effective field theory (new Lorentz structures)
  • simplified models, UV complete theories

Rescaling Standard Model Higgs couplings

Higgs-gluon coupling effective theory

Parametrize Higgs-gluon coupling by dim.-7 operators (Gracey '02; Neill '09; Germer '07)

\[\begin{multline*} \mathcal{L}_{eff}=\frac{\color{black}{C_{1}}}{\color{red}{\Lambda}}HF_{\mu\nu}^{a}F^{a\,\mu\nu} +\frac{\color{black}{C_{2}}}{\color{red}{\Lambda^{3}}}HD_{\alpha}F_{\mu\nu}^{a}D^{\alpha}F^{a\,\mu\nu}+\frac{\color{black}{C_{3}}}{\color{red}{\Lambda^{3}}}HF_{\nu}^{a\,\mu}F_{\sigma}^{b\,\nu}F_{\mu}^{c\,\sigma}f^{abc}\\ +\frac{\color{black}{C_{4}}}{\color{red}{\Lambda^{3}}}HD^{\alpha}F_{\alpha\nu}^{a}D_{\beta}F^{a\,\beta\nu}+\frac{\color{black}{C_{5}}}{\color{red}{\Lambda^{3}}}HF_{\alpha\nu}^{a}D^{\nu}D^{\beta}F_{\beta}^{a\,\alpha} \\ \equiv \frac{\color{black}{C_{1}}}{\color{red}{\Lambda}} \mathcal{O}_1 + \frac{\color{black}{C_{2}}}{\color{red}{\Lambda^3}} \mathcal{O}_2 + \frac{\color{black}{C_{3}}}{\color{red}{\Lambda^3}} \mathcal{O}_3 + \frac{\color{black}{C_{4}}}{\color{red}{\Lambda^3}} \mathcal{O}_4 + \frac{\color{black}{C_{5}}}{\color{red}{\Lambda^3}} \mathcal{O}_5 \end{multline*} \]

  • Compute kinematical distributions

Higgs+Jet: Higgs \(p_T\) distribution

Normalization to corresponding part of cross-section: only shape matters here; coefficients \(C_i\) a priori unknown. (Harlander, Neumann '13)

Are we ready for high \(p_T\) Higgs?



HTL: Heavy Top Limit

leading term in asymptotic expansion in \(\color{blue}{1/m_t^k}\)

  • About 1% error for total inclusive cross-section (NNLO):
    • asymptotic expansions (Harlander, Ozeren '09; Pak, Rogal, Steinhauser '09)
    • exact high energy limit (Marzani, Ball, Del Duca, Forte, Vincini '08 '09; Harlander, Mantler, Marzani, Ozeren '10; Del Duca, Kilgore, Oleari, Schmidt, Zeppenfeld '03)

Higgs+jet at NLO

Asymptotic expansion in \(m_{\text{top}} \gg \Lambda\)

V. A. Smirnov 90's

\[ F(\Gamma) \to \sum_\gamma \mathcal{T} F(\gamma) \star F(\Gamma\backslash\gamma) \]

  • Two loop diagram (\(\hat{s}, m_H^2, m_t^2\)) reduces to tadpole integrals with vanishing external momenta and massless integrals
  • Automatized setup expq2e (Harlander, Seidensticker, Steinhauser '98; Steinhauser '01)

Validity for exclusive production?

Asymptotic expansion in \((\Lambda/m_t)^k\), where \(\Lambda\in\{m_H, \sqrt{\hat{s}}, p_T, \dots\}\)
  • LO studies (Ellis, Hinchliffe, Soldate '88; Baur, Glover '90; Del Duca, Kilgore, Oleari, Schmidt, Zeppenfeld '01; Alwall, Li, Maltoni '12; Bagnaschi, Degrassi, Slavich, Vicini '12)

Mass effects in Higgs+jet at NLO: Beyond the HTL

  • Our goal was to estimate effects and assess the validty of the HTL
    (Harlander, TN, Ozeren, Wiesemann '12; TN, Wiesemann '14)

Mass effects in Higgs+jet at NLO: Beyond the HTL

  • We can improve the prediction, if the asymptotic expansion "converges"

Beyond the asymptotic expansion

  • just asymptotic expansion in two loop virtual corrections

  • massive one loop real emission contributions exactly (H + 4 partons)

Generalized unitarity cuts

  • Unitarity cuts pioneered in the mid 90's (Bern, Dixon, Dunbar, Kosower '94)
  • Generalized unitarity: multiple cuts, complex momenta, D dimensions
    (Britto, Cachazo, Feng '05; Anastasiou, Britto, Feng, Kunszt, Mastrolia '06; Forde '07;)
  • lead to the NLO one-loop revolution: i.e. BlackHat, GoSam, HelacNLO, MadLoop, OpenLoops, Rocket, …

Generalized unitarity cuts

  • Generalized unitarity: multiple cuts, complex momenta, D dimensions
    (Britto, Cachazo, Feng '05; Anastasiou, Britto, Feng, Kunszt, Mastrolia '06; Forde '07;)
  • lead to the NLO one-loop revolution: i.e. BlackHat, GoSam, HelacNLO, MadLoop, OpenLoops, Rocket, …

  • Our setup: S@M (Maître, Mastrolia '07) + boxes, triangles (rat pieces) via D-dim gen. unitarity (Badger '09), bubbles via Stokes' Theorem spinor-integration (Mastrolia '09)

Best fixed order Higgs high \(p_T\) spectrum

  • efficiently implemented in MCFM (POWHEG-BOX soon)

    • similar recent study "green curve with parton showers": Frederix, Frixione, Vryonidou, Wiesemann '16

    Best fixed order Higgs high \(p_T\) spectrum

    Improvement over full asymptotic expansion

    (Neumann, Williams 1605.XXXXX)

    In progress: Things to do for 1605.XXXX

    • "fix" LO virt interference, check scale dependence
    • consider other observables (jet \(p_T\), jet inclusive, Higgs \(p_T\) inclusive, etc.)
    • take into account NNLO K-factor (or similar)
    • consider improvements for BSM searches (?)