1
$\begingroup$

Physicists at Moriond 2021 reported New results on theoretically clean observables in rare $B$-meson decays from LHCb 3.1 sigma away from the SM prediction of lepton universality in the $B+→K+μ+μ- $vs. $B+→K+e+e-$ comparison (i.e. there is apparent lepton flavor universality violation (LFV)). Muons are less common than electrons in the decay products. The ratios seem to be coming up at about 86% of the expected Standard Model number of muon pair decays relative to electron-positron decays.

The simplest answer in the Standard Model would seem be that there are two processes.

One produces equal numbers of electron-positron and muon pair decays together with a positively charged kaon in each case, as expected. The pre-print linked above states this about this process:

The B+ hadron contains a beauty antiquark, b, and the K+ a strange antiquark, s, such that at the quark level the decay involves a b → s transition. Quantum field theory allows such a process to be mediated by virtual particles that can have a physical mass larger than the mass difference between the initial- and final-state particles. In the SM description of such processes, these virtual particles include the electroweak-force carriers, the γ, W± and Z bosons, and the top quark. Such decays are highly suppressed and the fraction of B+ hadrons that decay into this final state (the branching fraction, B) is of the order of 10−6.

A second process with a branching fraction of about 1/6th that of the primary process produces a positively charged kaon together with an electromagnetically neutral particle that has more than about 1.22 MeV of mass (enough to decay to a positron-electron pair), but less than about 211.4 MeV mass necessary to produce a muon pair when it decays.

It turns out that there is exactly one such known particle fundamental or composite, specifically, a neutral pion, with a mass of about 134.9768(5) MeV. About 98.8% of the time, a πº it decays to a pair of photons and that decay would be ignored as the end product doesn't match the filtering criteria. But about 1.2% of the time, it decays to an electron-positron pair together with a photon, and all other possible decays are vanishingly rare by comparison.

So, we need a decay of a B+ meson to a K+ meson and a neutral pion with a branching fraction of about (10-6) * (1/6) * (1/0.012)= 1.4 * 10-5.

It turns out that B+ mesons do indeed decay to K+ mesons and neutral pions with a branching fraction of 1.29(5) * 10-5 which is almost exactly what it needs to be to produce the apparent violation of lepton universality.

It also appears to me that the theoretical calculation of the K+µ+µ- to K+e+e- ratio isn't considering this decay, although it seems mind boggling to me that so many physicists in such a carefully studied process would somehow overlook the B+ --> K+πº decay channel impact on their expected outcome, which is the obvious way to reverse engineer the process.

I looked at the methodology section of the paper on event selection and didn't see anything showing any kind of event selection that would weed out πº decays to electron-positron pairs.

Does this make sense, or am I missing something?

$\endgroup$

1 Answer 1

4
$\begingroup$

I am not an expert in this area, but I see that they apply a cut on the invariant mass-squared of the two leptons: $$1.1 < q^2 < 6.0\,\mathrm{GeV}^2/c^4.$$

The pion mass (squared) is way outside this cut, and so I suppose that the contribution from that decay mode doesn't pollute their measurement, though they don't say so explicitly. [Note that on page 3 they do discuss the value of the cut for excluding other resonances such as the $J/\psi$ or $\phi(1020$)]

$\endgroup$

Your Answer

By clicking “Post Your Answer”, you agree to our terms of service and acknowledge you have read our privacy policy.

Not the answer you're looking for? Browse other questions tagged or ask your own question.