85 research outputs found

    Minimal Z' models and the early LHC

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    We consider a class of minimal extensions of the Standard Model with an extra massive neutral gauge boson Z'. They include both family-universal models, where the extra U(1) is associated with (B-L), and non-universal models where the Z' is coupled to a non-trivial linear combination of B and the lepton flavours. After giving an estimate of the range of parameters compatible with a Grand Unified Theory, we present the current experimental bounds, discussing the interplay between electroweak precision tests and direct searches at the Tevatron. Finally, we assess the discovery potential of the early LHC.Comment: 6 pages, 2 figures. Talk given at the 2nd Young Researchers Workshop "Physics Challenges in the LHC Era", Frascati, May 10 and 13, 201

    Relevance of the decay W' → Wγ at the early LHC

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    We study, employing an effective approach, the early LHC phenomenology of an isospin-singlet W', focusing on the process pp → W' → Wγ. We discuss how observation of this decay would be a hint of the compositeness of the resonance, and present an estimate of the experimental reach in the 7TeV LHC run

    (Dys)Zphilia or a custodial breaking Higgs at the LHC

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    Electroweak precision measurements established that custodial symmetry is preserved to a good accuracy in the gauge sector after electroweak symmetry breaking. However, recent LHC results might be interpreted as pointing towards Higgs couplings that do not respect such symmetry. Motivated by this possibility, we reconsider the presence of an explicitly custodial breaking coupling in a generic Higgs parameterization. After briefly commenting on the large UV sensitivity of the T parameter to such a coupling, we perform a fit to results of Higgs searches at LHC and Tevatron, and find that the apparent enhancement of the ZZ channel with respect to WW can be accommodated. Two degenerate best-fit points are present, which we label `Zphilic' and `dysZphilic' depending on the sign of the hZZ coupling. Finally we highlight some measurements at future linear colliders that may remove such degeneracy.Comment: 16 pages, 10 figure

    The Dark Penguin Shines Light at Colliders

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    Collider experiments are one of the most promising ways to constrain Dark Matter (DM) interactions. For several types of DM-Standard Model couplings, a meaningful interpretation of the results requires to go beyond effective field theory, considering simplified models with light mediators. This is especially important in the case of loop-mediated interactions. In this paper we perform the first simplified model study of the magnetic dipole interacting DM, by including the one-loop momentum-dependent form factors that mediate the coupling -- given by the Dark Penguin -- in collider processes. We compute bounds from the monojet, monophoton, and diphoton searches at the 88 and 1414 TeV LHC, and compare the results to those of direct and indirect detection experiments. Future searches at the 100100 TeV hadron collider and at the ILC are also addressed. We find that the optimal search strategy requires loose cuts on the missing transverse energy, to capture the enhancement of the form factors near the threshold for on-shell production of the mediators. We consider both minimal models and models where an additional state beyond the DM is accessible. In the latter case, under the assumption of anarchic flavor structure in the dark sector, the LHC monophoton and diphoton searches will be able to set much stronger bounds than in the minimal scenario. A determination of the mass of the heavier dark fermion might be feasible using the MT2M_{T2} variable. In addition, if the Dark Penguin flavor structure is almost aligned with that of the DM mass, a displaced signal from the decay of the heavier dark fermion into the DM and photon can be observed. This allows us to set constraints on the mixings and couplings of the model from an existing search for non-pointing photons.Comment: 32 pages + appendices and references, 22 figure

    Charged Composite Scalar Dark Matter

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    We consider a composite model where both the Higgs and a complex scalar χ\chi, which is the dark matter (DM) candidate, arise as light pseudo Nambu-Goldstone bosons (pNGBs) from a strongly coupled sector with TeV scale confinement. The global symmetry structure is SO(7)/SO(6)SO(7)/SO(6), and the DM is charged under an exact U(1)DM⊂SO(6)U(1)_{\rm DM} \subset SO(6) that ensures its stability. Depending on whether the χ\chi shift symmetry is respected or broken by the coupling of the top quark to the strong sector, the DM can be much lighter than the Higgs or have a weak-scale mass. Here we focus primarily on the latter possibility. We introduce the lowest-lying composite resonances and impose calculability of the scalar potential via generalized Weinberg sum rules. Compared to previous analyses of pNGB DM, the computation of the relic density is improved by fully accounting for the effects of the fermionic top partners. This plays a crucial role in relaxing the tension with the current DM direct detection constraints. The spectrum of resonances contains exotic top partners charged under the U(1)DMU(1)_{\rm DM}, whose LHC phenomenology is analyzed. We identify a region of parameters with f=1.4  TeVf = 1.4\; \mathrm{TeV} and 200  GeV≲mχ≲400  GeV200\;\mathrm{GeV} \lesssim m_\chi \lesssim 400\;\mathrm{GeV} that satisfies all existing bounds. This DM candidate will be tested by XENON1T in the near future.Comment: 36 pages + appendices and references, 10 figures. v2: minor modifications, references added. Matches version published in JHE

    Strong tW Scattering at the LHC

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    Deviations of the top electroweak couplings from their Standard Model values imply that certain amplitudes for the scattering of third generation fermions and longitudinally polarized vector bosons or Higgses diverge quadratically with momenta. This high-energy growth is a genuine signal of models where the top quark is strongly coupled to the sector responsible for electroweak symmetry breaking. We propose to profit from the high energies accessible at the LHC to enhance the sensitivity to non-standard top-ZZ couplings, which are currently very weakly constrained. To demonstrate the effectiveness of the approach, we perform a detailed analysis of tW→tWtW \to tW scattering, which can be probed at the LHC via pp→ttˉWjpp\to t\bar{t}Wj. By recasting a CMS analysis at 8 TeV, we derive the strongest direct bounds to date on the ZttZtt couplings. We also design a dedicated search at 13 TeV that exploits the distinctive features of the ttˉWjt\bar{t}Wj signal. Finally, we present other scattering processes in the same class that could provide further tests of the top-Higgs sector.Comment: 37 pages, 10 figures; v2: minor improvements in the discussion, references added. Matches version published in JHE

    Lifting degeneracies in Higgs couplings using single top production in association with a Higgs boson

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    Current Higgs data show an ambiguity in the value of the Yukawa couplings to quarks and leptons. Not so much because of still large uncertainties in the measurements but as the result of several almost degenerate minima in the coupling profile likelihood function. To break these degeneracies, it is important to identify and measure processes where the Higgs coupling to fermions interferes with other coupling(s). The most prominent example, the decay of h→γγh \to \gamma \gamma, is not sufficient to give a definitive answer. In this Letter, we argue that tt-channel single top production in association with a Higgs boson, with h→bbˉh\to b\bar b, can provide the necessary information to lift the remaining degeneracy in the top Yukawa. Within the Standard Model, the total rate is highly reduced due to an almost perfect destructive interference in the hard process, Wb→thW b \rightarrow t h. We first show that for non-standard couplings the cross section can be reliably computed without worrying about corrections from physics beyond the cutoff scale Λ≳10 TeV\Lambda\gtrsim 10\,\mathrm{TeV}, and that it can be enhanced by more than one order of magnitude compared to the SM. We then study the signal pp→thj(b) p p \rightarrow t h j (b) with 3 and 4 bb's in the final state, and its main backgrounds at the LHC. We find the 8 TeV run dataset to be sensitive to the sign of the anomalous top Yukawa coupling, while already a moderate integrated luminosity at 14 TeV should lift the degeneracy completely.Comment: 17 pages, 7 figures. v2: inclusive signal cross sections at NLO in QCD added; new comment on sensitivity of the analysis to t tbar h process. Matches version accepted by JHE
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