EW001 $S, T, U$
Peskin-Takeuchi oblique electroweak parameters Status SUBTLETY-ADDED VERIFIED High Code: NO Priority Medium
Why this constrains the RS scan
Bulk RS models generically shift \(S\) through mixing of the SM electroweak
bosons with KK gauge modes, and shift \(T\) when custodial symmetry is broken
by gauge, Higgs, or fermion embeddings. PDG summarizes the warped contribution
as \(S\simeq 30 v^2/M_{\rm KK}^2\) and quotes \(S\leq0.18\) at 95\%
probability as implying \(M_{\rm KK}\gtrsim3.2\,\mathrm{TeV}\). These bounds
are orthogonal to the catalog's \(\Delta F=2\) constraints, but they test the
same KK spectrum and localization choices before flavor observables are even
evaluated.
What's changed since the original paper
Relative to the CFW baseline, arXiv:0804.1954, the important change is not a
new LEP run but a much more mature global-fit environment: Higgs and top inputs
are measured directly, full two-loop and selected higher-order SM calculations
are included, and PDG now presents both \(U=0\) and floating-\(U\) oblique fits.
The 2022 CDF \(W\)-mass result created a distinct scenario in which \(T\) or
\(U\) can be pulled positive; the 2025 PDG review treats that impact as a
global-fit issue rather than replacing the main STU table with the CDF-only
preference.
Validity and model dependence
The STU language is cleanest for heavy, approximately universal new physics
whose leading effects are vacuum-polarization corrections. It is less complete
when vertex corrections, non-universal fermion couplings, light new states, or
SMEFT flat directions are numerically important. In RS applications, custodial
protection, brane kinetic terms, Higgs localization, and vector-like fermion
embeddings can change the translation from a fitted \(S,T,U\) point to a KK
mass bound.
In custodial RS, reduced \(Z b_L b_L\) pressure can reshuffle which EW
observable is most discriminating; quote RS bounds only after specifying
custodial protection, fermion embeddings, and brane kinetic terms.
Code coverage in this repo
NO. Greps over
quarkConstraints/, qcd/,
flavorConstraints/, neutrinos/, yukawa/,
warpConfig/, solvers/, scanParams/, and
tests/ found no S/T/U, oblique, EWPO, or W-mass-fit implementation.
Only generic electroweak constants and VEV comments surfaced, for example
qcd/constants.py:11, qcd/running.py:3,
quarkConstraints/qcd\_running.py:99, yukawa/neutrino.py:14,
and yukawa/charged\_lepton.py:11.Implementation difficulty
HIGH. A production constraint would need a new electroweak precision
likelihood, correlation handling for the PDG/GFitter/HEPfit fit conventions,
and RS matching from the gauge and fermion KK spectra to vacuum-polarization
self energies or equivalent SMEFT operators. This is a new electroweak
mode/matching calculation, not a reuse of the existing \(\Delta F=2\) basis.
Reason: A live EW001 constraint needs a new electroweak precision likelihood plus RS matching from gauge/fermion KK spectra to vacuum-polarization self energies or SMEFT bosonic operators. This is outside the existing $\Delta F = 2$ basis and requires new electroweak mode/matching calculations and correlated global-fit handling.
Key references
pdg\_2025\_electroweak\_stu;
gfitter\_oblique\_parameters;
hepfit\_deblas\_2022\_cdf\_stu;
hepfit\_precision\_ew\_page;
peskin\_takeuchi\_1992\_oblique;
cfw\_2008\_rs\_flavor.