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G. Bélanger

Publications and source records attributed to G. Bélanger.

25 records · Page 2Linked to original sources

Invisible Decays of the Supersymmetric Higgs and Dark Matter

We discuss effects of the light sparticles on decays of the lightest Higgs in a supersymmetric model with nonuniversal gaugino masses at the high scale, focusing on the `invisible' decays into neutralinos. These can impact significanlty the discovery possibilities of the lightest Higgs at the LHC. We show that due to these decays, there exist regions of the $M_2-μ$ space where the B.R. $(h \to γγ)$ becomes dangerously low even after imposing the LEP constraints on the sparticle masses, implying a possible preclusion of its discovery in the $γγ$ channel. We find that there exist regions in the parameter space with acceptable relic density and where the ratio ${B.R. (h \to γγ)_{SUSY} \over B.R. (h \to γγ)_{SM}}$ falls below 0.6, implying loss of signal in the $γγ$ channel. These regions correspond to $\tilde χ_1^+, \tilde χ_2^0$ masses which should be accessible already at the Tevatron. Further we find that considerations of relic density put lower limit on the U(1) gaugino mass parameter $M_1$ independently of $μ, \tan β$ and $m_0$.

hep-ph↗

The Higgs Working Group: Summary Report (2001)

Report of the Higgs working group for the Workshop `Physics at TeV Colliders', Les Houches, France, 21 May - 1 June 2001. It contains 7 separate sections: A. Theoretical Developments B. Higgs Searches at the Tevatron C. Experimental Observation of an invisible Higgs Boson at LHC D. Search for the Standard Model Higgs Boson using Vector Boson Fusion at the LHC E. Study of the MSSM channel $A/H \to ττ$ at the LHC F. Searching for Higgs Bosons in $t\bar t H$ Production G. Studies of Charged Higgs Boson Signals for the Tevatron and the LHC

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Associated stop Higgs Production at the Linear Collider and Extraction of the stop Parameters

We calculate stop stop Higgs production at the linear collider. Combining the measurements from the pair production of the lightest stop and that of the mass of the Higgs we show how, in a scenario where only the lightest stop and the lightest Higgs were accessible, one could extract the mass of the heavier stop and infer some useful information on the SUSY parameters.

hep-ph↗

Semi-leptonic four-fermion final states in polarised γγreactions: Exact results vs an improved narrow width approximation

We calculate the process $γγ\rightarrow e^- \barν_e u \bar{d}$ with the full set of Feynman diagrams. We consider different implementations of the $W$ width and different combinations of the photon polarisations. The results of an improved narrow width approximation based on $γγ\rightarrow W^+ W^-$ with full spin-correlations that takes into account different angular cuts as well as cuts on the invariant masses are compared to those of the complete calculation.

hep-ph↗

Effects of Non-Standard Tri-linear Couplings in Photon-Photon Collisions: I. $γγ\to W^+ W^-$

The effect of anomalous couplings in $γγ\to W^+ W^-$ is studied for different energies of the $γγ$ mode of the next linear collider. The analysis based on the maximum likelihood method exploits the variables in the four-fermion semi-leptonic final state. Polarised differential cross sections based on the complete set of diagrams for these channels with the inclusion of anomalous couplings are used and compared to an approximation based on $γγ\to W^+ W^-$ with full spin correlations. To critically compare these results with those obtained in $e^+ e^-$ we perform an analysis based on the complete calculation of the four-fermion semi-leptonic final state. The anomalous couplings that we consider are derived from the next-to-leading order operators in the non-linear realisation of symmetry breaking.

hep-ph↗

Inverse Neutrinoless Double Beta Decay Revisited

We critically reexamine the prospects for the observation of the $ΔL=2$ lepton-number-violating process $\eeWW$ using the $e^-e^-$ option of a high-energy $e^+e^-$ collider (NLC). We find that, except in the most contrived scenarios, constraints from neutrinoless double beta decay render the process unobservable at an NLC of $\sqrt{s}<2$ TeV. Other $ΔL=2$ processes such as $\ggllww$, $\egnllw$, $\eennll$ ($\ell=μ,τ$), and $\egeww$, which use various options of the NLC, require a $\sqrt{s}$ of at least 4 TeV for observability.

hep-ph↗