Abstract:We present a unified analysis of the two main production processes of vector boson pairs at the CERN LHC, VV-fusion and qq annihilation, in a minimal strongly interacting electroweak symmetry breaking sector. Using a unitarized electroweak chiral Lagrangian formalism and modeling the final V L V L strong rescattering effects by a form factor, we describe qq annihilation processes in terms of the two chiral parameters that govern elastic V L V L scattering. Depending on the values of these two chiral parameters… Show more
In the absence of a Higgs boson, the perturbative description of the Standard Model ceases to make sense above a TeV. Heavy spin-1 fields coupled to W and Z bosons can extend the validity of the theory up to higher scales. We carefully identify regions of parameter space where a minimal addition -a single spin-1 SU(2) custodial -triplet resonance -allows one to retain perturbative control in all channels. Elastic scattering of longitudinal W and Z bosons alone seems to permit a very large cut-off beyond the Naive Dimensional Analysis expectation. We find however that including scattering of the spin-1 resonances then leads to an earlier onset of strong coupling. Most importantly for LHC searches, we define a self-consistent set-up with a well-defined range of validity without recourse to unitarization schemes whose physical meaning is obscure. We discuss the LHC phenomenology and the discovery reach for these electroweak resonances and mention the possibility of a nightmare scenario with no Higgs nor resonance within the LHC reach. Finally, we discuss the effects of parity breaking in the heavy resonance sector which reduces the contributions to the S parameter.
In the absence of a Higgs boson, the perturbative description of the Standard Model ceases to make sense above a TeV. Heavy spin-1 fields coupled to W and Z bosons can extend the validity of the theory up to higher scales. We carefully identify regions of parameter space where a minimal addition -a single spin-1 SU(2) custodial -triplet resonance -allows one to retain perturbative control in all channels. Elastic scattering of longitudinal W and Z bosons alone seems to permit a very large cut-off beyond the Naive Dimensional Analysis expectation. We find however that including scattering of the spin-1 resonances then leads to an earlier onset of strong coupling. Most importantly for LHC searches, we define a self-consistent set-up with a well-defined range of validity without recourse to unitarization schemes whose physical meaning is obscure. We discuss the LHC phenomenology and the discovery reach for these electroweak resonances and mention the possibility of a nightmare scenario with no Higgs nor resonance within the LHC reach. Finally, we discuss the effects of parity breaking in the heavy resonance sector which reduces the contributions to the S parameter.
“…The old electroweak chiral Lagrangian (ECL) [4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21], based on standard chiral perturbation theory (ChPT) of QCD [46][47][48][49], assumed a Higgsless model, but solved the problems that the Higgs was intended for by supposing a strongly interacting regime for the EWSBS instead. In view that the h has been found, it can be extended to include the new Higgs-like particle found at the LHC (refs.…”
Section: Chapter 2 Chiral Ew Lagrangianmentioning
confidence: 99%
“…[1][2][3]). The tools of Effective Chiral Lagrangians and unitarization procedures will be used, and the old Higgsless Electroweak Chiral Lagrangian [4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21](EChL) will be extended to accommodate a Higgs-like boson at ∼ 125 GeV. Since the discovery of the Higgs-like boson at the LHC, this field has received increasing attention [22][23][24][25][26][27][28][29][30][31][32][33].…”
“…The operators O i include the complete set of operators defined, e.g., in [1,19,20]. We will be interested in WW scattering and work in the strict custodial limit.…”
Section: Constraining the Effective Lagrangian Coefficientsmentioning
confidence: 99%
“…Neglecting the gauge boson mass (quite justified at 2 TeV), unitarity requires the form factor to obey the following relation within a vector-dominance region [20] ImF V ðsÞ ¼ t…”
A diboson excess has been observed-albeit with very limited statistical significance-in WW, WZ, and ZZ final states at the LHC experiments using the accumulated 8 TeV data. Assuming that these signals are due to resonances resulting from an extended symmetry breaking sector in the standard model and exact custodial symmetry, we determine using unitarization methods the values of the relevant low-energy constants in the corresponding effective Lagrangian. Unitarity arguments also predict the widths of these resonances. We introduce unitarized form factors to allow for a proper treatment of the resonances in Monte Carlo generators and a more precise comparison with experiment.
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