L008 $\mathcal{B}(\tau^-\to e^-\gamma)$
Tau to e $\gamma$ charged-lepton-flavor-violating dipole decay Status REVIEWED VERIFIED Medium Code: NO Priority Medium
PDG / equivalent values
| Observable | Value | Year | Experiment / source | Provenance |
|---|---|---|---|---|
| Branching fraction upper limit for $\tau^- \to $ e- $\gamma$ | 3.3e-8 | 2025 | Particle Data Group 2025 PDGLive tau decay summary, PDGID S035.32 | source ↑ |
| Branching fraction upper limit for $\tau \to $ e $\gamma$ | 3.3e-8 | 2010 | BaBar Collaboration full-data tau -> l gamma search | source ↑ |
| Branching fraction upper limit for $\tau^+- \to $ e+- $\gamma$ | 5.6e-8 | 2021 | Belle Collaboration full-data tau -> l gamma search | source ↑ |
| Projected branching-fraction sensitivity for $\tau \to $ e $\gamma$ | ? | 2019 | Belle II Physics Book | source ↑ |
Why this constrains the RS scan
In warped lepton-flavor extensions, this mode constrains brane-localized or
loop-induced charged-lepton dipoles with a \(\tau e\) flavor spurion. It is
not a constraint on the current quark \(\Delta F=2\) scan, but it is a useful
catalog entry for any future charged-lepton implementation because alignment
that suppresses \(\mu\to e\gamma\) need not suppress the tau-to-electron
transition in the same way. The Perez--Randall warped-neutrino source gives
the lepton-MFV/GIM-like assumptions under which charged-lepton flavor
violation is controlled.
What's changed since the original paper
Relative to the arXiv:0804.1954 RS flavor baseline, the main experimental
development is the BaBar 2010 full-data result, which remains the canonical
PDG value for \(\tau\to e\gamma\)
(
L008.yaml:pdg\_or\_equivalent.primary\_experiment;
L008.yaml:pdg\_or\_equivalent.rs\_context). Belle later repeated the
search with its full \(988\,{\rm fb}^{-1}\) data set and found no significant
excess, setting the weaker electron-mode limit \(5.6\times10^{-8}\) at
\(90\%\) C.L.
(L008.yaml:pdg\_or\_equivalent.recent\_belle\_cross\_check). The author
pass found no Belle II measurement superseding the BaBar/PDG bound; the
sidecar records only the \(50\,{\rm ab}^{-1}\),
\(1.2\times10^{-8}\) Belle II prospect
(L008.yaml:pdg\_or\_equivalent.belle\_ii\_projection).Validity and model dependence
Experimentally this is a clean null search for charged-lepton flavor
violation, with a negligible Standard Model rate. Its RS interpretation is
model-dependent: the bound constrains a dipole coefficient only after choosing
the lepton localization, flavor symmetry, Yukawa normalization, and KK-mass
convention. The catalog should therefore classify it as robust
experimentally, but lepton-extension-only and dipole-model-dependent for this
repo.
Code coverage in this repo
NO. The required catalog grep over
quarkConstraints/,
qcd/, flavorConstraints/, neutrinos/,
yukawa/, warpConfig/, solvers/,
scanParams/, and tests/ found no \(\tau\to e\gamma\)
implementation. The adjacent code surface is only \(\mu\to e\gamma\):
flavorConstraints/muToEGamma.py:1 documents that process,
flavorConstraints/muToEGamma.py:75 defines
check\_mu\_to\_e\_gamma, and scanParams/scan.py:523 and
scanParams/scan.py:524 call that checker in scans. Those lines are
reusable design evidence, not L008 coverage.Implementation difficulty
MEDIUM. A future implementation can reuse the existing LFV dipole
pattern, but it must generalize the flavor indices and rate normalization from
\(\mu\to e\gamma\) to tau decays, add a tau-sector branching-ratio limit, and
decide whether the same RS lepton-spurion assumptions apply. No new hadronic
matrix elements, lattice inputs, or QCD running are needed.
Reason: The repo has an adjacent $\mu \to e \gamma$ dipole pattern, but L008 needs a generalized lepton-dipole observable with tau-e flavor indices, tau lifetime/normalization, and a process-specific branching-ratio limit. No new hadronic matrix elements, lattice inputs, or QCD running are needed.
Key references
Process-local source keys before bibliography consolidation:
PDG2025\_TauEGamma, BaBar2010\_TauLGamma,
Belle2021\_TauLGamma, BelleIIPhysicsBook2019\_TauLFV,
CFW2008\_RSWarpedFlavor, and
PerezRandall2008\_WarpedNeutrinos.