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Abstract
A measurement of the phase difference between
the short- and long-distance contributions to the B+ →
K +μ+μ− decay is performed by analysing the dimuon mass
distribution. The analysis is based on pp collision data corresponding
to an integrated luminosity of 3 fb−1 collected by
the LHCb experiment in 2011 and 2012. The long-distance
contribution to the B+ → K +μ+μ− decay is modelled as
a sum of relativistic Breit–Wigner amplitudes representing
different vector meson resonances decaying to muon pairs,
each with their own magnitude and phase. The measured
phases of the J/ψ and ψ(2S) resonances are such that the
interference with the short-distance component in dimuon
mass regions far from their pole masses is small. In addition,
constraints are placed on the Wilson coefficients, C9 and C10,
and the branching fraction of the short-distance component
is measured.
the short- and long-distance contributions to the B+ →
K +μ+μ− decay is performed by analysing the dimuon mass
distribution. The analysis is based on pp collision data corresponding
to an integrated luminosity of 3 fb−1 collected by
the LHCb experiment in 2011 and 2012. The long-distance
contribution to the B+ → K +μ+μ− decay is modelled as
a sum of relativistic Breit–Wigner amplitudes representing
different vector meson resonances decaying to muon pairs,
each with their own magnitude and phase. The measured
phases of the J/ψ and ψ(2S) resonances are such that the
interference with the short-distance component in dimuon
mass regions far from their pole masses is small. In addition,
constraints are placed on the Wilson coefficients, C9 and C10,
and the branching fraction of the short-distance component
is measured.
Original language | English |
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Journal | European Physical Journal C: Particles and Fields |
Volume | 77 |
Issue number | 161 |
DOIs | |
Publication status | Published - 16 Mar 2017 |
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