Little-Higgs corrections to precision data after LEP2
Guido Marandella, Christian Schappacher, Alessandro Strumia
TL;DR
The paper reevaluates little-Higgs corrections to precision electroweak data across several global-symmetry models, showing that most corrections are universal and can be captured by the four oblique parameters $\\hat{S}$, $\\hat{T}$, $W$, and $Y$, with LEP2 data tightening the bounds. It introduces a practical method to compute these universal effects by integrating out heavy vector bosons and demonstrates it on multiple models, including the littlest Higgs variants, the SO(9) model, and SU(6)/Sp(6) constructions, while also treating non-universal Z' contributions via an approximate four-parameter encoding. The results yield lower bounds on the symmetry-breaking scale $f$ of typically a few TeV, highlighting a residual little-hierarchy problem and significant fine-tuning to reproduce the electroweak scale. The work also shows how non-universal Z' effects can be mapped onto the same parameter set using leptonic data, and discusses prospects for testing these scenarios with future precision measurements at e^+e^- colliders.
Abstract
We reconsider little-Higgs corrections to precision data. In five models with global symmetries SU(5), SU(6), SO(9) corrections are (although not explicitly) of `universal' type. We get simple expressions for the Shat, That, W, Y parameters, which summarize all effects. In all models Shat > (W+Y)/2 and That, W, Y\ge 0. Results differ from previous analyses, which are sometimes incomplete, sometimes incorrect, and because we add LEP2 e ebar --> f fbar cross sections to the data set. Depending on the model the constraint on f ranges between 2 and 20 TeV. We next study the `simplest' little-Higgs model (and propose a new related model) which is not `universal' and affects precision data due to the presence of an extra Z' vector. By restricting the data-set to the most accurate leptonic data we show how corrections to precision data generated by a generic Z' can be encoded in four effective Shat, That, W, Y parameters, giving their expressions.
