K010 $\mathcal{B}(K_S\to\pi^0 e^+e^-)$
Short-lived neutral-kaon rare semileptonic electron mode Status REVIEWED VERIFIED High Code: NO Priority Low
PDG / equivalent values
| Observable | Value | Year | Experiment / source | Provenance |
|---|---|---|---|---|
| $BR(K_S \to $ pi0 e+ e-, $m_{ee}$ > 0.165 GeV) | 3.0e-9 branching fraction | 2026 | Particle Data Group 2026 pdgLive listing S012.10 / NA48 | source ↑ |
| $BR(K_S \to $ pi0 e+ e-), full kinematic region | 5.8e-9 branching fraction | 2026 | Particle Data Group 2026 pdgLive listing S012.10 / NA48 | source ↑ |
| NA48/1 observed signal candidates | 7 events | 2003 | NA48/1 2003 arXiv hep-ex/0309075 | source ↑ |
| NA48/1 expected background | 0.15 events | 2003 | NA48/1 2003 arXiv hep-ex/0309075 | source ↑ |
Why this constrains the RS scan
This mode probes \(s\to d e^+e^-\) semileptonic neutral-current structure,
not the \(\Delta F=2\) kaon-mixing lane already implemented in the repository.
In warped or anarchic-flavor models it is sensitive, through a hadronic
long-distance amplitude, to flavor-changing \(Z\), photon-penguin, and heavy
neutral-gauge effects. Its most immediate catalog role is as an experimental
normalization for the indirect-CP part of \(K_L\to\pi^0 e^+e^-\), so it should
be kept distinct from short-distance theory prefactors or NDA normalizations.
What's changed since the original paper
No post-2008 measurement was found that supersedes the NA48/1 value used by
PDG. The important developments are interpretive: the rare-kaon Snowmass
white paper emphasizes \(K_{L,S}\to\pi^0\ell^+\ell^-\) branching ratios and
\(q^2\) distributions as new-physics probes, with correlations to
\(\varepsilon'/\varepsilon\), \(\varepsilon_K\), and \(\Delta M_K\). The
modern literature also treats this \(K_S\) input as part of the indirect-CP
normalization for the \(K_L\) modes rather than as a standalone clean Wilson
coefficient bound (
aebischer\_buras\_kumar\_2022\_arxiv.txt,
isidori\_smith\_unterdorfer\_2004\_arxiv.txt).Validity and model dependence
Class: long-distance-limited rare kaon decay. The measured partial branching
fraction is robust, but the full-kinematic number is model-dependent because
it assumes a vector matrix element and a unit form factor. A model constraint
must specify whether it uses the directly measured \(m_{ee}>0.165\) GeV region
or the extrapolated total rate, and whether it predicts the chiral
long-distance amplitude or only a short-distance \(s\to d e^+e^-\) Wilson
coefficient.
Code coverage in this repo
NO. Focused greps over
quarkConstraints/, qcd/,
flavorConstraints/, neutrinos/, yukawa/,
warpConfig/, solvers/, scanParams/, and
tests/ found no \(K_S\to\pi^0 e^+e^-\), \(S012.10\),
\(a_S\), or \(s\to d e^+e^-\) implementation. The nearest kaon coverage is
\(\Delta F=2\): quarkConstraints/deltaf2.py:209 starts the default
neutral-meson-mixing inputs, quarkConstraints/deltaf2.py:755
evaluates \(\Delta m_K\), and
quarkConstraints/modern/phenomenology.py:23 lists only
\(\varepsilon_K\), \(K\), \(B_d\), \(B_s\), and \(D0\) policy systems.Implementation difficulty
HIGH. Production integration would need a new \(\Delta S=1\)
semileptonic rare-kaon observable, Wilson normalization for \(s\to d e^+e^-\),
and a documented treatment of the \(K_S\) form factor or a conservative
experimental-input-only interpretation. The existing SLL/SLR/VLL/VRR/LR
\(\Delta F=2\) basis does not cover this decay.
Key references
Process-local source keys before bibliography consolidation:
PDG2026:K010, NA482003:KSPi0EE,
IsidoriSmithUnterdorfer2004:KPi0LL,
AebischerBurasKumar2022:RareKaons, and
CFW2008:RSFlavor.