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Updated: May 6, 2026

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Search for the lepton-flavor-violating decays B(s)0→e(±)μ(∓) and B0→e(±)μ(∓)
1Nikhef National Institute for Subatomic Physics, Amsterdam, The Netherlands.
Physical Review Letters
|October 22, 2013
Summary
The LHCb experiment searched for rare B-meson decays violating lepton flavor, setting stringent new limits on branching fractions. These findings constrain new physics models, including Pati-Salam leptoquarks.
Area of Science:
- High Energy Physics
- Particle Physics
- Beyond Standard Model Physics
Background:
- Lepton flavor violation (LFV) is a key indicator of new physics beyond the Standard Model.
- Searches for LFV decays of B-mesons provide sensitive probes of new particles and interactions.
- Previous experiments have set limits on LFV decays such as B(s)0→e(±)μ(∓) and B0→e(±)μ(∓).
Purpose of the Study:
- To search for the lepton-flavor-violating decays B(s)0→e(±)μ(∓) and B0→e(±)μ(∓).
- To set new upper limits on the branching fractions of these rare decays.
- To constrain the masses of hypothetical Pati-Salam leptoquarks.
Main Methods:
- Analysis of a data sample corresponding to an integrated luminosity of 1.0 fb(-1) of proton-proton collisions at √s=7 TeV.
- Utilizing the LHCb detector to identify and reconstruct B(s)0 and B0 meson decays.
- Statistical analysis to compare observed candidates with background expectations and set upper limits.
Main Results:
- The observed number of candidate events for both B(s)0→e(±)μ(∓) and B0→e(±)μ(∓) decays is consistent with background.
- Upper limits on branching fractions are set at B(B(s)0→e(±)μ(∓))<1.1(1.4)×10(-8) and B(B0→e(±)μ(∓))<2.8(3.7)×10(-9) at 90% (95%) confidence level.
- These limits are approximately a factor of 20 lower than those from previous experiments.
Conclusions:
- The stringent new limits significantly improve upon previous measurements for these LFV decays.
- The results place strong constraints on new physics scenarios, particularly those involving leptoquarks.
- Lower bounds on Pati-Salam leptoquark masses are established at M(LQ)(B(s)0→e(±)μ(∓))>101 TeV/c(2) and M(LQ)(B0→e(±)μ(∓))>126 TeV/c(2) at 95% C.L., a factor of 2 higher than previous bounds.
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