Search for an invisibly decaying Z′Z^{\prime} boson at Belle II in e+e−→μ+μ−(e±μ∓)e^+ e^- \to μ^+ μ^- (e^{\pm} μ^{\mp}) plus missing energy final states

preprint2020arXivOpen access
Belle II CollaborationI. AdachiP. AhlburgH. AiharaN. AkopovA. AloisioN. Anh KyD. M. AsnerH. AtmacanT. AushevV. AushevT. AzizV. BabuS. BaehrP. BambadeSw. BanerjeeV. BansalM. BarrettJ. BaudotJ. BeckerP. K. BeheraJ. V. BennettE. BernieriF. U. BernlochnerM. BertemesM. BessnerS. BettariniF. BianchiD. BiswasA. BozekM. BračkoP. BranchiniR. A. BriereT. E. BrowderA. BudanoL. BurmistrovS. BussinoM. CampajolaL. CaoG. CasarosaC. CecchiD. ČervenkovM. -C. ChangR. CheaibV. ChekelianY. Q. ChenY. -T. ChenB. G. CheonK. ChilikinK. ChoS. ChoS. -K. ChoiS. ChoudhuryD. CinabroL. CoronaL. M. CremaldiS. CunliffeT. CzankF. DattolaE. De La Cruz-BureloG. De NardoM. De NuccioG. De PietroR. de SangroM. DestefanisS. DeyA. De Yta-HernandezF. Di CapuaZ. DoležalI. Domínguez JiménezT. V. DongK. DortD. DossettS. DubeyS. DuellG. DujanyS. EidelmanM. EliachevitchJ. E. FastT. FerberD. FerlewiczG. FinocchiaroS. FioreA. FodorF. FortiB. G. FulsomE. GanievM. Garcia-HernandezR. GargV. GaurA. GazA. GellrichJ. GemmlerT. GeßlerR. GiordanoA. GiriB. GobboR. GodangP. GoldenzweigB. GolobP. GomisW. GradlE. GrazianiD. GreenwaldY. GuanC. HadjivasiliouS. HalderT. HaraO. HartbrichK. HayasakaH. HayashiiC. HeartyM. T. HedgesI. Heredia de la CruzM. Hernández VillanuevaA. HershenhornT. HiguchiE. C. HillM. HoekC. -L. HsuY. HuT. IijimaK. InamiG. IngugliaJ. Irakkathil JabbarA. IshikawaR. ItohY. IwasakiW. W. JacobsD. E. JaffeE. -J. JangH. B. JeonS. JiaY. JinC. JooK. K. JooJ. KahnH. KakunoA. B. KaliyarJ. KandraG. KaryanY. KatoT. KawasakiB. H. KimC. -H. KimD. Y. KimK. -H. KimS. -H. KimY. K. KimY. KimT. D. KimmelH. KindoC. KleinwortP. KodyšT. KogaS. KohaniI. KomarovS. KorparN. KovalchukT. M. G. KraetzschmarP. KrižanR. KroegerP. KrokovnyT. KuhrJ. KumarM. KumarR. KumarK. KumaraS. KurzA. KuzminY. -J. KwonS. LacapraraC. La LicataL. LanceriJ. S. LangeK. LautenbachI. -S. LeeS. C. LeeP. LeitlD. LevitL. K. LiY. B. LiJ. LibbyK. LieretL. Li GioiZ. LiptakQ. Y. LiuD. LiventsevS. LongoT. LuoY. MaedaM. MaggioraE. ManoniS. MarcelloC. MarinasA. MartiniM. MasudaT. MatsudaK. MatsuokaD. MatvienkoF. MeggendorferJ. C. MeiF. MeierM. MerolaF. MetznerM. MilesiC. MillerK. MiyabayashiH. MiyakeR. MizukK. AzmiG. B. MohantyT. MoonT. MoriiH. -G. MoserF. MuellerF. J. MüllerTh. MullerG. MuroyamaR. MussaE. NakanoM. NakaoM. NayakG. NazaryanD. NeverovC. NiebuhrN. K. NisarS. NishidaK. NishimuraM. NishimuraB. OberhofK. OgawaY. OnishchukH. OnoY. OnukiP. OskinH. OzakiP. PakhlovG. PakhlovaA. PaladinoA. PantaE. PaoloniH. ParkB. PaschenA. PasseriA. PathakS. PaulT. K. PedlarI. PeruzziR. PeschkeR. PestotnikM. PiccoloL. E. PiilonenV. PopovC. PrazE. PrencipeM. T. PrimM. V. PurohitP. RadosR. RasheedS. ReiterM. RemnevP. K. ResmiI. Ripp-BaudotM. RitterG. RizzoL. B. RizzutoS. H. RobertsonD. Rodríguez PérezJ. M. RoneyC. RosenfeldA. RostomyanN. RoutG. RussoD. SahooY. SakaiS. SandilyaA. SangalL. SanteljP. SartoriY. SatoV. SavinovB. ScavinoJ. SchuelerC. SchwandaR. M. SeddonY. SeinoA. SelceK. SenyoC. SfientiC. P. ShenJ. -G. ShiuB. ShwartzA. SibidanovF. SimonR. J. SobieA. SofferA. SokolovE. SolovievaS. SpataroB. SpruckM. StaričS. StefkovaZ. S. StottlerR. StroiliJ. StrubeM. SumihamaT. SumiyoshiD. J. SummersS. Y. SuzukiM. TabataM. TakizawaU. TamponiS. TanakaK. TanidaN. TaniguchiP. TarasF. TenchiniE. TorassaK. TrabelsiT. TsuboyamaM. UchidaK. UngerY. UnnoS. UnoY. UshirodaS. E. VahsenR. van TonderG. S. VarnerK. E. VarvellA. VinokurovaL. VitaleA. VossenM. WakaiH. M. WakelingW. Wan AbdullahC. H. WangM. -Z. WangA. WarburtonM. WatanabeJ. WebbS. WehleC. WesselJ. WiechczynskiH. WindelE. WonB. YabsleyS. YamadaW. YanS. B. YangH. YeJ. H. YinM. YonenagaC. Z. YuanY. YusaL. ZaniZ. ZhangV. ZhilichQ. D. ZhouX. Y. ZhouV. I. Zhukova

Abstract

Theories beyond the standard model often predict the existence of an additional neutral boson, the Z′Z^{\prime}. Using data collected by the Belle II experiment during 2018 at the SuperKEKB collider, we perform the first searches for the invisible decay of a Z′Z^{\prime} in the process e+e−→μ+μ−Z′e^+ e^- \to μ^+ μ^- Z^{\prime} and of a lepton-flavor-violating Z′Z^{\prime} in e+e−→e±μ∓Z′e^+ e^- \to e^{\pm} μ^{\mp} Z^{\prime}. We do not find any excess of events and set 90\% credibility level upper limits on the cross sections of these processes. We translate the former, in the framework of an Lμ−LτL_μ-L_τ theory, into upper limits on the Z′Z^{\prime} coupling constant at the level of 5×10−25 \times 10^{-2} -- 11 MZ′≤6M_{Z^\prime}\leq 6 GeV/c2c^2.

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