K017 $R_K = \Gamma(K^+ \to e^+ \nu_e(\gamma)) / \Gamma(K^+ \to \mu^+ \nu_\mu(\gamma))$
Charged-kaon leptonic lepton-universality ratio Status REVIEWED VERIFIED Medium Code: NO Priority Low
PDG / equivalent values
| Observable | Value | Year | Experiment / source | Provenance |
|---|---|---|---|---|
| PDG API / PDG Live summary S010R28 | 2.488 dimensionless decay-rate ratio | 2025 | PDG API / PDG Live summary S010R28 | source ↑ |
| NA62 Collaboration, Phys. Lett. B 719 (2013) 326 | 2.488 dimensionless decay-rate ratio | 2013 | NA62 Collaboration, Phys. Lett. B 719 (2013) 326 | source ↑ |
| KLOE Collaboration, Eur. Phys. J. C 64 (2009) 627 | 2.493 dimensionless decay-rate ratio | 2009 | KLOE Collaboration, Eur. Phys. J. C 64 (2009) 627 | source ↑ |
| Cirigliano and Rosell, JHEP 0710 (2007) 005 | 2.477 dimensionless decay-rate ratio | 2007 | Cirigliano and Rosell, JHEP 0710 (2007) 005 | source ↑ |
Why this constrains the RS scan
This is not a neutral-meson \(\Delta F=2\) observable and does not probe the
existing quark scan's KK-gluon mixing lane directly. Its value is that the
ratio cancels the common \(V_{us}\), \(f_K\), and much of the kaon-rate
normalization, leaving a helicity-suppressed charged-current LFU test
(
FlaviaNet:Kaon2010).
Nonminimal warped models with lepton localization, heavy neutral leptons,
nonunitary charged currents, charged scalars, or nonuniversal \(W\)-coupling
shifts can modify \(K_{e2}\) relative to \(K_{\mu2}\). In a quark-only RS
interpretation it should therefore be cataloged as a lepton-extension or
charged-current diagnostic, not as a hard bound on the current anarchic
quark fit.What's changed since the original paper
The 2008 CFW baseline predates the precision \(R_K\) consolidation and did
not make this charged-current LFU ratio a central RS constraint
(
CsakiFalkowskiWeiler:RSFlavor2008). Since then, KLOE published a
precise inclusive measurement in 2009 (KLOE:RK2009), the FlaviaNet
kaon working group consolidated post-2008 kaon-decay inputs in 2010
(FlaviaNet:Kaon2010), and NA62 superseded earlier charged-kaon data
with its 2007--2008 data set in 2013 (NA62:RK2013). The modern PDG
average is driven by those post-2008 measurements. The theory reference value
was already clean before 2008, but the experimental precision now makes
\(R_K\) a useful null test for scalar or right-handed charged-current effects
that evade many hadronic uncertainties.Validity and model dependence
As a measured ratio, \(R_K\) is robust and experimentally clean, provided the
radiative convention is kept fixed: the PDG/NA62 ratio includes internal
bremsstrahlung, while direct-emission radiation is separated. Its mapping
onto this repository's default model is model-dependent. A minimal quark
flavor scan with no nonstandard charged-current lepton sector has no direct
parameter controlling this observable, whereas a 5D lepton extension or
charged-scalar completion could generate visible effects through chirality-
enhanced scalar amplitudes or lepton-nonuniversal \(W\) couplings.
Code coverage in this repo
NO. The required coverage greps across
quarkConstraints/,
qcd/, flavorConstraints/, neutrinos/,
yukawa/, warpConfig/, solvers/,
scanParams/, and tests/ find no \(K^+\to e^+\nu\),
\(K^+\to\mu^+\nu\), \(K_{\ell2}\), or \(R_K\) implementation. The nearest
surfaces are the \(\Delta F=2\) default inputs in
quarkConstraints/deltaf2.py:209 and the modern policy fence
quarkConstraints/modern/phenomenology.py:23, which enumerates only
\(\varepsilon_K\), \(K\), \(B_d\), \(B_s\), and \(D0\).Implementation difficulty
MEDIUM. A catalog-to-code implementation would need a new
charged-current leptonic-decay observable, including the SM amplitude,
radiative-convention bookkeeping, and whatever BSM operator basis the PI wants
to expose. The ratio avoids new lattice matrix elements, but it is not covered
by the existing \(\Delta F=2\) SLL/SLR/VLL/VRR/LR machinery.
Reason: Needs a new charged-current leptonic-decay observable and BSM operator/matching convention; no new lattice input is needed because the ratio cancels f_K, but existing $\Delta F = 2$ machinery does not cover it.
Key references
Process-local reference keys before bibliography consolidation:
PDG2025:K017RK, NA62:RK2013, KLOE:RK2009, CiriglianoRosell:RKSM2007,
FlaviaNet:Kaon2010, and CsakiFalkowskiWeiler:RSFlavor2008.