K003 $\mathrm{Re}(\varepsilon'/\varepsilon)$
Direct CP violation in K $ \to \pi \pi$ Status REVIEWED VERIFIED High Code: NO Priority Medium
PDG / equivalent values
| Observable | Value | Year | Experiment / source | Provenance |
|---|---|---|---|---|
| $Re(\epsilon'/\epsilon$) | $Re(\epsilon'/\epsilon) = 0.00166 +/- 0.00023 = (16.6 +/- 2.3) x 10^-4$ | 2025 | Particle Data Group pdgLive K0 listing, row S013EPS | source ↑ |
Why this constrains the RS scan
Unlike \(\varepsilon_K\), this is a \(\Delta S=1\) nonleptonic observable.
It tests CP-odd short-distance contributions to the \(K\to\pi\pi\) amplitudes
after they are filtered through long-distance QCD. In warped or composite
flavor models with anarchic Yukawas, the dangerous effects are not the
repo's current neutral-meson-mixing operators but new penguin, scalar/tensor,
and dipole structures. BSM master-formula work identifies strong sensitivity
to electroweak left-right penguin \(Q_8\), QCD penguin \(Q_6\), and
chromo-magnetic \(O_{8g}\)-type operators, making the channel a natural
stress test for UV completions with non-minimal chirality structure.
What's changed since the original paper
The experimental average has not been replaced by a newer kaon experiment, but
KTeV's final \(K\to\pi\pi\) result was published after the CFW-era baseline.
The main post-2008 changes are theoretical. RBC/UKQCD produced a
physical-kinematics lattice calculation of \(A_0\) and \(\varepsilon'\), with
\(\mathrm{Re}(\varepsilon'/\varepsilon)=
21.7(2.6)(6.2)(5.0)\times10^{-4}\). Aebischer, Bobeth, and Buras then
reanalysed the ratio with NNLO electroweak-penguin corrections and ChPT
isospin-breaking inputs, obtaining
\((17.4\pm6.1)\times10^{-4}\) in the octet treatment and
\((13.9\pm5.2)\times10^{-4}\) in the nonet treatment. In parallel, 2019
BSM master-formula papers organized the \(\Delta S=1\) operator dependence
in WET/SMEFT language rather than treating \(\varepsilon'/\varepsilon\) as a
single phenomenological number.
Validity and model dependence
As a catalog constraint, \(K003\) is highly informative but not plug-and-play.
The experimental number is cleanly established, while the SM subtraction and
BSM interpretation depend on hadronic matrix elements, isospin breaking,
operator matching, and RG evolution. It should be classified as a
theory-limited, model-dependent \(\Delta S=1\) amplitude constraint rather
than a robust tree-level exclusion like the current \(\Delta F=2\) kaon lane.
Code coverage in this repo
NO. Greps over
quarkConstraints/, qcd/,
flavorConstraints/, neutrinos/, yukawa/,
warpConfig/, solvers/, scanParams/, and
tests/ found no direct implementation of
\(\varepsilon'/\varepsilon\), \(K\to\pi\pi\), \(\Delta S=1\), \(Q_6\),
\(Q_8\), or \(O_{8g}\). The nearby kaon code is explicitly a
\(\Delta F=2\) benchmark slice in quarkConstraints/deltaf2.py:1,
with default inputs for \(\varepsilon_K\) at
quarkConstraints/deltaf2.py:209 and an
\(\varepsilon_K\) evaluator at quarkConstraints/deltaf2.py:729.
The modern policy surface likewise enumerates only
\(\varepsilon_K\), \(K\), \(B_d\), \(B_s\), and \(D^0\) systems at
quarkConstraints/modern/phenomenology.py:23.
Linked evidence (opens GitHub blob at flavor-catalog-website/2026q2):
- No direct K003 matches from the focused grep command; exit status 1.
- quarkConstraints/deltaf2.py:1 implements a Delta F = 2 benchmark observable layer, not Delta S = 1 K -> pi pi amplitudes.
- quarkConstraints/deltaf2.py:209 lists epsilon_K, B_d, B_s, and D mixing inputs.
- quarkConstraints/deltaf2.py:729 defines evaluate_epsilon_k, not epsilon'/epsilon.
- quarkConstraints/modern/phenomenology.py:23 enumerates only epsilon_K, K, B_d, B_s, and D0 policy systems.
Implementation difficulty
HIGH. A production constraint would require a new \(\Delta S=1\)
operator basis, matching from the warped/composite UV model to WET/SMEFT
coefficients, RG running to hadronic scales, and lattice/ChPT inputs for
\(K\to\pi\pi\) matrix elements. The current \(\Delta F=2\) VLL/VRR/LR
machinery cannot be reused as a direct evaluator.
Reason: Requires new $\Delta S = 1$ WET/SMEFT matching, RG evolution, $K \to \pi \pi$ matrix elements, and treatment of electroweak/QCD penguin plus chromomagnetic operators; the repo's $\Delta F = 2$ machinery is not a direct evaluator.
Key references
Local source keys:
pdg\_live\_S013\_20260516,
pdg\_live\_S013EPS\_datablock\_20260516, ktev\_2011,
na48\_2002, rbc\_ukqcd\_2020,
aebischer\_buras\_2020, bsm\_master\_2019,
bsm\_anatomy\_2019, and cfw\_2008.