2026/01/11 by LHCb collaboration, R. Aaij, Carlos Abellán Beteta +1212 · 2 voices
Physics and Astronomy · #Neutrino Physics Research #Particle physics theoretical and experimental studies #Quantum Chromodynamics and Particle Interactions #hep-ex
paper · pdf · doi:10.1103/pl88-4435
published as Phys. Rev. Lett. 137 (2026) 051801 · All figures and tables, along with any supplementary material and additional information, are available at https://lhcb-glance.cern.ch/alcm/public/analysis/full-details/5370
arxiv published 2026/01/11 · openalex publication_date 2026/03/24 · openalex created_date 2026/03/25 · arxiv created 2026/07/29 · arxiv updated 2026/07/29 · openalex updated_date 2026/07/30
A search for the rare decay B+ → Λp μ+ μ- is performed using proton-proton collision data recorded by the LHCb experiment at a center-of-mass energy of √(s)= 13 TeV, corresponding to an integrated luminosity of 5.4 fb-1. An excess of events is found with respect to the background-only expectation, with a signal significance of 3.5 standard deviations, in the low invariant-mass region of m( Λp)<2.8 GeV/c2. The branching fraction is measured to be \cal B\rm low(B+→ Λp μ+ μ-)=(1.70 +0.65-0.56(\rm stat) ± 0.17(\rm syst) ± 0.14(\rm ext)) × 10-8, where the last uncertainty is due to external inputs on \cal B(B+→J/ψ Λp)× \cal B(J/ψ→μ+μ-). With no significant signal observed in the high m( Λp) region above 2.8 GeV/c2, an upper limit is set to be \cal B\rm high(B+→ Λp μ+ μ-)<2.8 (3.7) × 10-9 at the 90% (95%) confidence level.