53 research outputs found

    S and T Parameters from a Light Nonstandard Higgs versus Near Conformal Dynamics

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    We determine the contribution to the SS and TT parameters coming from extensions of the standard model featuring a light nonstandard-like Higgs particle. We neatly separate, using the Landau gauge, the contribution from the purely nonstandard Higgs sector, from the one due to the interplay of this sector with the standard model. If the nonstandard Higgs sector derives from a new type of near conformal dynamics, the formalism allows to precisely link the intrinsic underlying contribution with the experimentally relevant parameters.Comment: 13 pages, 3 figure

    An Effective Higgsless Theory: Satisfying Electroweak Constraints and a Heavy Top Quark

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    The main challenge faced by Higgsless models of electroweak symmetry breaking is to reconcile the experimental constraints imposed by the precision electroweak data and the top quark phenomenology with the unitarity constraints imposed by longitudinal gauge boson scattering amplitudes. In this paper we expand on previous work, giving details of how delocalized fermions can be used to adjust the SS parameter to zero, while keeping the TT and UU parameters naturally suppressed. We also show that it is possible to obtain the top quark mass, without affecting the delay of unitarity violation of the W+W−→W+W−W^+ W^-\to W^+W^- scattering amplitude, by separating the mass scales of the fermion sector (1/Rf1/R_f) from that of the gauge sector (1/Rg1/R_g). The fermion sector scale 1/Rf1/R_f is only weakly constrained by unitarity of the ttˉ→W+W−t\bar{t}\to W^+ W^- scattering amplitude; thus the ratio Rg/RfR_g/R_f can be quite large, and the top mass can be easily achieved. Anomalous right-handed couplings involving the third generation quarks also avoid constraints from experimental data if 1/Rf1/R_f is sufficiently large.Comment: 26 pages, JHEP forma

    Probing Near-Conformal Technicolor through Weak Boson Scattering

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    The recently observed boson at 125 GeV could be a light composite scalar from near-conformal technicolor dynamics: a technicolor Higgs. If this is the case, unitarization of longitudinal weak boson scattering amplitudes, which is due to exchanges of the Higgs and spin-one vector technimesons, is expected to occur in a strong regime, with saturation of the unitarity bounds. This implies that pp→VVjjpp \to V V jj processes, where VV is either a WW or a ZZ boson, are enhanced, relative to the standard model. We show that this allows probing near-conformal technicolor for couplings and masses of the spin-one resonances which are not directly accessible for direct Drell-Yan production.Comment: 19 pages, 4 figure

    WW Scattering in Walking Technicolor

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    We analyze the WW scattering in scenarios of dynamical electroweak symmetry breaking of walking technicolor type. We show that in these theories there are regions of the parameters space allowed by the electroweak precision data, in which unitarity violation is delayed at tree level up to around 3-4 TeV without the inclusion of any sub-TeV resonances.Comment: 2 Columns RevTeX, 10 pages, 9 Figure

    Unitarity in Technicolor

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    We investigate the longitudinal WWWW scattering in models of dynamical electroweak symmetry breaking featuring a spin one axial and vector state and a composite Higgs. We also investigate the effects of a composite spin two state which has the same properties of a massive graviton. Any model of dynamical electroweak symmetry breaking will feature, depending on the dynamics, some or all these basic resonances as part of the low energy spectrum. We suggest how to take limits in the effective Lagrangian parameter space to reproduce the dynamics of different types of underlying gauge theories, from the traditional Technicolor models to the newest ones featuring nearly conformal dynamics. We study the direct effects of a light composite Higgs and the indirect ones stemming from the presence of a light axial resonance on the longitudinal WWWW scattering.Comment: 23 pages, 5 figure

    Technicolor Dark Matter

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    Dark Matter candidates are natural in Technicolor theories. We introduce a general framework allowing to predict signals of Technicolor Dark Matter at colliders and set constraints from earth based experiments such as CDMS and XENON. We show that the associate production of the composite Higgs can lead to relevant signals at the Large Hadron Collider.Comment: RevTeX, 4 pages, 6 figures. New figure one with added the projected data for superCDM

    Constraining Walking and Custodial Technicolor

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    We show how to constrain the physical spectrum of walking technicolor models via precision measurements and modified Weinberg sum rules. We also study models possessing a custodial symmetry for the S parameter at the effective Lagrangian level - custodial technicolor - and argue that these models cannot emerge from walking type dynamics. We suggest that it is possible to have a very light spin-one axial vector boson. However, in the walking dynamics the associated vector boson is heavy while it is degenerate with the axial in custodial technicolor.Comment: Two columns, RevTex, 4 pages, 5 eps file

    125 GeV Higgs from a not so light Technicolor Scalar

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    Assuming that the observed Higgs-like resonance at the Large Hadron Collider is a technicolor isosinglet scalar (the technicolor Higgs), we argue that the standard model top-induced radiative corrections reduce its dynamical mass towards the desired experimental value. We then discuss conditions for the spectrum of technicolor theories to feature a technicolor Higgs with the phenomenologically required dynamical mass. We use scaling laws coming from modifying the technicolor matter representation, number of technicolors, techniflavors as well as the number of doublets gauged under the electroweak theory. Finally we briefly summarize the potential effects of walking dynamics on the technicolor Higgs.Comment: ReVTex, 15 pages, 3 figures. Version to match the published on

    Constraints on Little Higgs with Fully-Radiative Electroweak Symmetry Breaking

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    In a recent paper, we introduced a new Little Higgs model, which contains the gauge structure SU(2)3×U(1)SU(2)^3\times U(1), embedded in an approximate global SO(5)×SO(5)SO(5)\times SO(5) symmetry. After breaking to the standard model, SU(2)L×U(1)YSU(2)_L \times U(1)_Y, this produces two heavy Z′Z^\prime bosons and two heavy W′±W^{\prime\pm} bosons, along with a single Standard Model-like Higgs scalar. The unique feature of the model was that it was possible to obtain electroweak symmetry breaking and a light Higgs mass entirely from perturbative loop contributions to the Higgs effective potential. In this paper we consider the electroweak constraints on this model, including tree and loop contributions to the universal oblique and non-oblique parameters, tree-level corrections to the ZWWZWW vertex, and tree and loop level corrections to ZbbˉZb\bar{b}. The most significant corrections are positive tree-level corrections to S^\hat{S} and negative fermion-loop corrections to T^\hat{T}, which require that the scale for the global symmetry breaking be ≳2\gtrsim2 TeV, depending on the top-quark mixing parameter and the extra gauge couplings. In addition, the loop corrections to ZbbˉZb\bar{b} contain a divergence that must be absorbed into the coefficient of a new operator in the theory. The finite part of this ZbbˉZb\bar{b} correction, however, is negligible.Comment: 28 pages, 16 figures, RevTeX forma
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