Baryogenesis from B Meson Oscillations

PHYSICAL REVIEW D 100, 075002 (2019) Baryogenesis from B meson oscillations † Ann E. Nelson * and Huangyu Xiao Department of Physics, University of Washington, Seattle, Washington 98195-1560, USA (Received 17 June 2019; published 1 October 2019) We show how CP violating B meson oscillations in conjunction with baryon number violating decays can generate the cosmological asymmetry between matter and antimatter, and explore the parameter space of a simple, self-contained model, which can be tested via exotic B meson decays, and via the charge asymmetry in semileptonic decays of neutral B mesons. DOI: 10.1103/PhysRevD.100.075002 I. INTRODUCTION visible matter-anti-matter asymmetry and asymmetric dark matter [6] via B-meson decays. In the present Baryogenesis—generating the cosmological asymme- work, we reexamine the simpler model of Ref. [4],and try between matter and antimatter—requires physics show that for a different parameter range that was not beyond the Standard Model (SM). The pioneering work considered in the previous work, baryon number vio- of Sakharov [1] found three necessary conditions: baryon B0 number violation, C and CP violation, and departure lating decays of mesons are allowed by experiment, from thermal equilibrium. Baryon number violation potentially observable, and could be the explanation for occurs nonperturbatively in the Standard Model [2]. baryogenesis. The baryogenesis scenario described here begins in the CP violation also occurs, however the standard model prenucleosynthesis early universe with the decays of CP violation appears to be too small to explain the a long lived scalar into b-quarks and antiquarks. These observed baryon asymmetry. Finally, the minimal decays are assumed to take place late enough and at Standard Model contains no mechanism for departure low enough temperature to allow hadronization, but from thermal equilibrium. before nucleosynthesis. Most of the b-quarks form B Recent work [3,4] has shown the possibility for low mesons. The neutral B mesons then oscillate and decay, energy baryogenesis via the oscillations of neutral sometimes to baryons or antibaryons, resulting in the hadrons, in conjunction with new sources of CP and observed asymmetry. baryon number violation. In Ref. [4], the oscillating Our model is similar to the one used in Ref. [5] to – hadrons were mesinos bound states of a quark and an produce the baryon asymmetry through oscillations of antisquark. In that work a relatively long-lived squark baryons [3,4], although even simpler. It is worth noting decayed into antiquarks via baryon number violating that even though we use a similar model, the parameter R-parity violating decays. A minimal model to capture space is different and we are less constrained from – this physics was studied in detail that model contained dinucleon decay. The mechanism we describe is similar “ ” three neutral Majorana fermions ( neutralinos )anda to the one found in a slightly more elaborate model [6], “ ” color triplet scalar ( squark ). The same model, in a which could generate a dark matter relic along with baryon different parameter region with lighter neutralinos, was number. In the current work we have no dark matter shown to lead to baryogenesis via potentially observ- sector. We assume that whatever the dark matter is, it is able baryon and CP violating neutral heavy flavor very weakly coupled and has no effect on baryogenesis. baryon oscillations [3,5]. A similar model, in which It would be a straightforward matter to include, for baryon number is conserved but also carried by dark instance, axion dark matter. Note that the presence of a matter, was shown to be capable of producing both the late decaying heavy particle can have an effect on the allowed axion parameter range and substructure [7]. *[email protected] This paper is organized as following: In Sec. II we give † [email protected] an overview of B meson physics and how it could be related to baryogenesis. A more detailed description of the model Published by the American Physical Society under the terms of and phenomenology is given in Sec. III. In Sec. IV we show the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to that the baryon asymmetry may be produced with para- the author(s) and the published article’s title, journal citation, meters which are allowed by experiment. In Sec. V we and DOI. Funded by SCOAP3. conclude and sketch ideas for future work. 2470-0010=2019=100(7)=075002(9) 075002-1 Published by the American Physical Society ANN E. NELSON and HUANGYU XIAO PHYS. REV. D 100, 075002 (2019) II. CHARGE ASYMMETRY IN OSCILLATING for baryogenesis is a new contribution to mixing in the Bs B-MESONS AND SIGN OF THE system. MATTER-ANTI-MATTER ASYMMETRY III. NEW PHENOMENOLOGY FROM We briefly review the physics of neutral B-meson OUR MODEL oscillations and describe how new physics in the decays A minimal renormalizable model for this baryogenesis and mixing can lead to baryogenesis. The oscillations are mechanism contains three new particles: One Majorana described by an effective 2 state Hamiltonian: fermion, χ, in the mass range 2–3 GeV, one new charge −1=3 color triplet scalar ϕ, with mass in the range 500 GeV Φ i MM12 i ΓΓ12 to 1.9 TeV, and a very weakly coupled particle, , which H ¼ M − Γ ¼ − : ð1Þ decays out of equilibrium into b-quarks and antiquarks. 2 MÃ M 2 ΓÃ Γ 12 12 The upper bound on the ϕ mass is from the need for a large enough branching ratio for exotic B meson decay, as we Here M and Γ are respectively the dispersive part and the explain later. Φ might be the inflaton or a string modulus. absorptive part of the transition amplitude. The CP violat- As Φ is very weakly coupled it is not experimentally ing phase argðΓ12=M12Þ is reparameterization invariant and accessible. Detailed computation shows that we need the observable in the semi-leptonic charge asymmetry of mass of Φ to be between 11 GeVand about a hundred GeV. neutral meson decays. This phase is crucial for our baryo- We note that it is to be expected that a scalar in this mass genesis mechanism, as it determines whether there are more range would mainly decay into b-quarks. A simple way to b quarks or b anti-quarks at the time of decay. With an achieve this goal is coupling Φ to the Higgs boson with a † asymmetry between b quarks and antiquarks, the baryon very small coupling constant g∶ΔL ¼ gΦH H. The number violating decays of the b quark into two lighter vacuum expectation value (VEV) of the Higgs boson antiquarks and a Majorana fermion, or the b anti-quark into would naturally give rise to gvΦh, which results in a tiny two quarks and a Majorana fermion can produce the amount of Φ-H mixing and a decay channel to b-quarks. observed matter antimatter asymmetry. In order for baryon The neutral Majorana fermion χ and color triplet ϕ will number violating decays to produce more matter than anti- interact with SU(2) singlet quarks through the following matter, there must be more b-antiquarks at the time of terms: decay. Because the semi-leptonic decays of b-antiquarks L ⊃− ϕÃ ¯ i cj − ϕχ¯ cj produce positively charged leptons, this baryogenesis int gij uRdR yj dR þ H:c: ð2Þ mechanism requires a positive charge asymmetry in either 0 B or Bs meson oscillations, or both. The charge asym- where i and j are flavor indices which run over the three metry depends on the phase of the absorptive term (Γ12) generations of up- and down-type quarks. χ relative to the dispersive term (M12) in B meson mixing. The Majorana fermion is neutral and its mass should be The magnitude of Γ12 and M12 are measured and are in greater than the mass difference between proton and electron, − 937 75 agreement with the Standard Model in both neutral meson mp me ¼ . MeV, otherwise this model will give systems. In the Standard Model, the phase argðΓ12=M12Þ is rise to proton decay [3].Themassofχ will be taken to be 0 – ϕ predicted to be very small for both the B and the Bs due to 2 3 GeV in this paper. Mediated by , the Majorana fermion the unitarity of the CKM matrix and the relatively small χ could decay to three quarks. The lifetime must be less than mass of the charm quark, leading to a very small prediction 0.1s to avoid spoiling successful BBN [8]. This requires that 5 2 for the charge asymmetry. Experimentally, the charge gijyj0 ≳ ð5 GeV=mχÞ ðmϕ=350 TeVÞ [5],withi ¼ u or c asymmetry has not yet been distinguished from zero in and j; j0 ¼ d or s. either system. The prediction in the standard model is that The colored scalar ϕ will either decay to antiquark pairs the charge asymmetry is negative for the B0 and positive or into χ plus a quark, and could appear in searches for dijet ϕ but very small for the Bs. Our detailed analysis will show resonances and jets and missing energy. The mass of that because more b quarks fragment into B0 mesons than should be at least about 500 GeV to pass collider Bs mesons, and because of the small size of the standard constraints [9]. There will also be many constraints from model asymmetry in Bs mesons, new physics in the mixing nucleon oscillations and dinucleon decays [5], which give amplitude may be needed for baryogenesis from B mesons. us upper bounds on various flavor combinations of the New physics which makes a small contribution to M12 and gij and yj couplings.

Load more