C005 $\mathcal{B}(D^0\to e^+e^-)$
Rare leptonic decay D0 $ \to $ e+ e- Status REVIEWED VERIFIED High Code: NO Priority Low
PDG / equivalent values
| Observable | Value | Year | Experiment / source | Provenance |
|---|---|---|---|---|
| BR(D0 $ \to $ e+ e-) | 7.9e-8 branching fraction | 2026 | PDG Live/API S032.39 | source ↑ |
| BR(D0 $ \to $ e+ e-) | 7.9e-8 branching fraction | 2010 | Belle Phys. Rev. D 81 (2010) 091102 / arXiv:1003.2345 | source ↑ |
| BR(D0 $ \to $ e+ e-) | 1.7e-7 branching fraction | 2012 | BABAR Phys. Rev. D 86 (2012) 032001 / arXiv:1206.5419 | source ↑ |
Why this constrains the RS scan
Anarchic warped models can induce up-sector flavor-changing neutral currents
through nonuniversal KK gauge couplings, flavor-violating \(Z\)-like effects,
Higgs/radion scalar exchange, or lepton-sector extensions
(
CsakiFalkowskiWeiler2008:CompositeFlavor). C005 therefore tests a
pure \(c\to u\) dilepton amplitude rather than the four-quark \(\Delta F=2\)
operator basis used for neutral \(D\)-mixing. For the current quark-only scan
it is a catalog and roadmap process; a live veto would need both the
\(c\to u\) current and electron-current normalization.What's changed since the original paper
The 2008 RS-flavor baseline predates the Belle and BaBar leptonic \(D^0\)
searches (
CsakiFalkowskiWeiler2008:CompositeFlavor). The main
post-2008 experimental development is Belle's 2010 improvement to the current
PDG limit, followed by BaBar's 2012 cross-check in a separate
\(e^+e^-\to c\bar c\) sample
(Belle2010:D0Ee, BaBar2012:D0EeMuMuEMu). Unlike C004,
which has newer hadron-collider dimuon searches, the accessed C005 PDG record
still uses the Belle result as the headline input. Rare-charm theory work
emphasizes that purely leptonic \(D^0\) limits are clean null tests
experimentally but require care when separating short-distance new physics from
long-distance charm dynamics
(BurdmanGolowichHewettPakvasa2002:RareCharm).Validity and model dependence
The upper limit itself is experimentally robust. Its interpretation as an RS
constraint is model dependent because the electron mode is helicity sensitive,
bremsstrahlung and electron identification enter the experimental acceptance,
and the Standard Model rare-charm amplitude is not a precision short-distance
prediction. A conservative use is an upper bound on additional short-distance
\(c\to u e^+e^-\) amplitudes in a specified operator basis, not a direct
subtraction against a sharply predicted Standard Model rate
(
BurdmanGolowichHewettPakvasa2002:RareCharm).Code coverage in this repo
NO. The author greps and a focused search for
D0.*e+e-, D0.*ee, c.?->.?u.*e, and
rare.?charm found no \(D^0\to e^+e^-\) implementation in
quarkConstraints/, qcd/, flavorConstraints/,
neutrinos/, yukawa/, warpConfig/,
solvers/, scanParams/, or tests/. Nearby hits are
not C005: \(D^0\) mixing is configured at
quarkConstraints/deltaf2.py:252 and evaluated at
quarkConstraints/deltaf2.py:941; the modern policy likewise lists
only \(D^0\) mixing at quarkConstraints/modern/phenomenology.py:23
and quarkConstraints/modern/phenomenology.py:668. The
\(\mu\to e\gamma\) dipole check at
flavorConstraints/muToEGamma.py:75 is a separate LFV observable.
Linked evidence (opens GitHub blob at flavor-catalog-website/2026q2):
- Focused exact C005 search returned no matches in the required implementation/test directories.
- quarkConstraints/deltaf2.py:252 and quarkConstraints/deltaf2.py:941 are D0 mixing hits, not D0 -> e+ e-.
- quarkConstraints/modern/phenomenology.py:23 and quarkConstraints/modern/phenomenology.py:668 are D0 mixing policy/evaluator hits, not rare leptonic charm.
- flavorConstraints/muToEGamma.py:75 is the separate mu -> e gamma LFV dipole check.
Implementation difficulty
HIGH. Production use would require a new \(\Delta C=1\) rare
leptonic module with vector, axial-vector, scalar, and pseudoscalar
normalizations, electron-mode acceptance conventions, and a documented
long-distance treatment. The existing \(\Delta F=2\) SLL/SLR/VLL/VRR/LR
basis is not enough.
Reason: $D0 \to e^+$ e- needs a new $\Delta C = 1$ rare leptonic observable with lepton-current normalization, electron-mode acceptance conventions, and long-distance treatment; the existing $\Delta F = 2$ basis does not cover it.
Key references
Process-local keys before bibliography consolidation:
PDG2026:D0Ee, Belle2010:D0Ee,
BaBar2012:D0EeMuMuEMu,
BurdmanGolowichHewettPakvasa2002:RareCharm, and
CsakiFalkowskiWeiler2008:CompositeFlavor. Numeric claims above are
tied to these sidecar source keys and local snapshots.