Beyond S, T and U
Ivan Maksymyk, C. P. Burgess, David London
TL;DR
The paper addresses the limitation of the traditional oblique-parameter framework ($S$, $T$, $U$) by extending it to lower-energy new physics that couples primarily to the gauge bosons. It develops a general treatment based on gauge-boson vacuum polarizations $\\delta \Pi_{ab}(q^2)$ and shows that neutral-current observables are described by $S$, $T$, $V$, and $X$, while a new parameter $W$ enters the $W$ width alongside $U$ when considering charged-current observables; mass-shell observables bring in the full set, including a distinct $W$-dependent contribution. An explicit degenerate heavy-fermion doublet example illustrates how $S$ dominates at large masses and how $V$, $W$, and $X$ behave, highlighting the diagnostic power of these extra parameters for inferring the scale and nature of new physics. The framework guides how precision electroweak data, especially with future measurements at LEP-200, can constrain or reveal light-to-intermediate mass new physics that couples to gauge bosons, providing a more complete and quantitative bridge between theory and experiment. Overall, the work extends the utility of oblique corrections to a broader mass range and emphasizes the role of additional parameters in capturing low-energy effects of new dynamics.
Abstract
The contribution to precision electroweak measurements due to TeV physics which couples primarily to the $W^\pm$ and $Z$ bosons may be parameterized in terms of the three `oblique correction' parameters, S, T and U. We extend this parameterization to physics at much lower energies, $\ge 100$ GeV, and show that in this more general case three more parameters are required (which we call V, W and X). Only two of these appear in neutral-current experiments, while the third new parameter enters into the $W^\pm$ width.
