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New Physics in $b \to s μ^+ μ^-$ after the Measurement of $R_{K^*}$ (1704.07397v3)

Published 24 Apr 2017 in hep-ph and hep-ex

Abstract: The recent measurement of $R_{K*}$ is yet another hint of new physics (NP), and supports the idea that it is present in $b\to s\mu+\mu-$ decays. We perform a combined model-independent and model-dependent analysis in order to deduce properties of this NP. Like others, we find that the NP must obey one of two scenarios: (I) $C_9{\mu\mu}({\rm NP}) < 0$ or (II) $C_9{\mu\mu}({\rm NP}) = - C_{10}{\mu\mu}({\rm NP}) < 0$. A third scenario, (III) $C_9{\mu\mu}({\rm NP}) = - C_{9}{\prime \mu\mu}({\rm NP})$, is rejected largely because it predicts $R_K = 1$, in disagreement with experiment. The simplest NP models involve the tree-level exchange of a leptoquark (LQ) or a $Z'$ boson. We show that scenario (II) can arise in LQ or $Z'$ models, but scenario (I) is only possible with a $Z'$. Fits to $Z'$ models must take into account the additional constraints from $B0_s$-${\bar B}0_s$ mixing and neutrino trident production. Although the LQs must be heavy, O(TeV), we find that the $Z'$ can be light, e.g., $M_{Z'} = 10$ GeV or 200 MeV.

Citations (193)

Summary

Overview of "New Physics in bb after the Measurement of RKR_{K^*}"

This paper conducts a thorough investigation into potential new physics (NP) underlying the observed anomalies in bsμ+μb \to s \mu^+\mu^- transitions, specifically following the measurement of RKR_{K^*} by the LHCb Collaboration. The measurement of RKR_{K^*}, which denotes the ratio of branching fractions of B0K0μ+μB^0 \to K^{*0} \mu^+ \mu^- over B0K0e+eB^0 \to K^{*0} e^+ e^-, reveals discrepancies from the Standard Model (SM) predictions that suggest lepton flavor universality violation.

Key Findings

The authors perform a comprehensive analysis, combining both model-independent and model-dependent approaches, to delineate the characteristics of NP in bb decays. They arrive at several conclusions:

  1. Scenarios of New Physics: The analysis indicates that NP must adhere to one of two scenarios:
    • Scenario I: C9μμ(NP)<0C_9^{\mu\mu}({\rm NP}) < 0
    • Scenario II: C9μμ(NP)=C10μμ(NP)<0C_9^{\mu\mu}({\rm NP}) = - C_{10}^{\mu\mu}({\rm NP}) < 0

A third scenario, (III) C9μμ(NP)=C9μμ(NP)C_9^{\mu\mu}({\rm NP}) = - C_{9}^{\prime \mu\mu}({\rm NP}), is ruled out primarily because it leads to theoretical predictions inconsistent with observed experimental results, notably predicting RK=1R_K = 1, contrary to the experimental data.

  1. Model Implications:
    • The simplest NP models, which involve the tree-level exchange of a leptoquark (LQ) or a ZZ' boson, support scenario (II) for both LQ and ZZ' models. Scenario (I) is feasible only with ZZ' boson exchange.
    • LQs are required to be heavy, approximately in the TeV range, while ZZ' bosons can be either heavy or light, with admissible masses as low as 10 GeV or as minuscule as 200 MeV.

Constraints and Implications

Additional constraints from Bs0B^0_s-mixingandneutrinotridentproductionnecessitatespecificpropertiesfromNPmodels:</p><ul><li>Heavy mixing and neutrino trident production necessitate specific properties from NP models:</p> <ul> <li>Heavy Z'modelsmusthaveaconsiderablecouplingtomuons,possiblyobservableinfutureexperimentsconcerningneutrinotridentproduction.</li><li>Light models must have a considerable coupling to muons, possibly observable in future experiments concerning neutrino trident production.</li> <li>Light Z'models,whichproposenovelopportunitiesindarkmatterandanomaliesrelatedtothemuonmagneticmoment,offeralternatepathwaysofinvestigation,potentiallyaddressingdiscrepanciesinotherflavorobservables.</li></ul><h3class=paperheadingid=futuredirections>FutureDirections</h3><p>Thepapersuggestsmultipledirectionsforfutureresearch:</p><ul><li>Exploringtheimplicationsoflight models, which propose novel opportunities in dark matter and anomalies related to the muon magnetic moment, offer alternate pathways of investigation, potentially addressing discrepancies in other flavor observables.</li> </ul> <h3 class='paper-heading' id='future-directions'>Future Directions</h3> <p>The paper suggests multiple directions for future research:</p> <ul> <li>Exploring the implications of light Z'modelsindetail,particularlytheireffectsatlowenergieswhichcouldsignificantlydeviatefromhighenergyexpectationsduetothe models in detail, particularly their effects at low energies which could significantly deviate from high-energy expectations due to the q^2dependence.</li><li>Detailedexperimentalinvestigationsintoneutrinotridentproductionmightunveilevidencedirectlypointingtothe dependence.</li> <li>Detailed experimental investigations into neutrino trident production might unveil evidence directly pointing to the Z'couplingstrengthspositedbythesemodels.</li><li>Continuedtheoreticalscrutinyofmodelindependentandmodeldependentfits,takingadvantageofupcominghighprecisionflavordata,couldfurtherrefineorchallengetheseconclusions.</li></ul><p>Insummary,thepapercarefullydelineatespotentialNPscenariosascribeabletoobservedmeasurements,advocatingforcontinuedexperimentalandmodelbasedexplorationintotheflavordynamicsgoverning coupling strengths posited by these models.</li> <li>Continued theoretical scrutiny of model-independent and model-dependent fits, taking advantage of upcoming high precision flavor data, could further refine or challenge these conclusions.</li> </ul> <p>In summary, the paper carefully delineates potential NP scenarios ascribeable to observed measurements, advocating for continued experimental and model-based exploration into the flavor dynamics governing b \to s$ transitions.