Search for B+→μ+ νμB^+ \to μ^+\, ν_μ and B+→μ+ NB^+ \to μ^+\, N with inclusive tagging

preprint2019arXivOpen access
M. T. PrimF. U. BernlochnerP. GoldenzweigM. HeckI. AdachiK. AdamczykH. AiharaS. Al SaidD. M. AsnerH. AtmacanV. AulchenkoT. AushevR. AyadV. BabuA. M. BakichV. BansalP. BeheraC. BeleñoV. BhardwajB. BhuyanT. BilkaJ. BiswalA. BobrovA. BozekM. BračkoN. BraunT. E. BrowderM. CampajolaL. CaoD. ČervenkovP. ChangV. ChekelianA. ChenB. G. CheonK. ChilikinH. E. ChoK. ChoY. ChoiS. ChoudhuryD. CinabroS. CunliffeZ. DoležalS. EidelmanD. EpifanovJ. E. FastT. FerberB. G. FulsomR. GargV. GaurA. GarmashA. GiriO. GrzymkowskaY. GuanJ. HabaT. HaraK. HayasakaH. HayashiiW. -S. HouT. IijimaK. InamiG. IngugliaA. IshikawaM. IwasakiY. IwasakiS. JiaY. JinD. JoffeK. K. JooA. B. KaliyarG. KaryanT. KawasakiH. KichimiC. KieslingC. H. KimD. Y. KimK. T. KimS. H. KimK. KinoshitaP. KodyšS. KorparD. KotchetkovP. KrižanR. KroegerP. KrokovnyT. KuhrR. KulasiriR. KumarT. KumitaA. KuzminY. -J. KwonK. LalwaniJ. S. LangeI. S. LeeJ. K. LeeJ. Y. LeeS. C. LeeP. LewisC. H. LiL. Li GioiJ. LibbyK. LieretD. LiventsevP. -C. LuT. LuoJ. MacNaughtonM. MasudaT. MatsudaD. MatvienkoM. MerolaF. MetznerK. MiyabayashiR. MizukG. B. MohantyR. MussaM. NakaoG. De NardoK. J. NathZ. NatkaniecM. NayakM. NiiyamaN. K. NisarS. NishidaK. NishimuraS. OgawaH. OnoY. OnukiP. PakhlovG. PakhlovaB. PalS. PardiH. ParkS. -H. ParkS. PatraS. PaulT. K. PedlarR. PestotnikL. E. PiilonenV. PopovE. PrencipeM. RitterA. RostomyanM. RozanskaG. RussoD. SahooY. SakaiL. SanteljV. SavinovO. SchneiderG. SchnellJ. SchuelerC. SchwandaY. SeinoK. SenyoM. E. SeviorV. ShebalinJ. -G. ShiuB. ShwartzF. SimonA. SokolovE. SolovievaM. StaričJ. F. StrubeM. SumihamaT. SumiyoshiW. SutcliffeM. TakizawaU. TamponiY. TaoF. TenchiniM. UchidaT. UglovY. UnnoS. UnoY. UshirodaY. UsovS. E. VahsenR. van TonderG. VarnerK. E. VarvellA. VinokurovaB. WangC. H. WangM. -Z. WangP. WangS. WatanukiE. WonS. B. YangH. YeJ. H. YinY. YusaZ. P. ZhangV. ZhilichV. ZhukovaV. Zhulanov

Abstract

We report the result for a search for the leptonic decay of B+→μ+ νμB^+ \to μ^+ \, ν_μ using the full Belle data set of 711 fb−1{}^{-1} of integrated luminosity at the Υ(4S)Υ(4S) resonance. In the Standard Model leptonic BB-meson decays are helicity and CKM suppressed. To maximize sensitivity an inclusive tagging approach is used to reconstruct the second BB meson produced in the collision. The directional information from this second BB meson is used to boost the observed μμ into the signal BB meson rest-frame, in which the μμ has a monochromatic momentum spectrum. Though its momentum is smeared by the experimental resolution, this technique improves the analysis sensitivity considerably. Analyzing the μμ momentum spectrum in this frame we find B(B+→μ+ νμ)=(5.3±2.0±0.9)×10−7\mathcal{B}(B^+ \to μ^+ \, ν_μ) = \left( 5.3 \pm 2.0 \pm 0.9 \right) \times 10^{-7} with a one-sided significance of 2.8 standard deviations over the background-only hypothesis. This translates to a frequentist upper limit of B(B+→μ+ νμ)<8.6×10−7\mathcal{B}(B^+ \to μ^+ \, ν_μ) < 8.6 \times 10^{-7} at 90% CL. The experimental spectrum is then used to search for a massive sterile neutrino, B+→μ+ NB^+ \to μ^+ \, N, but no evidence is observed for a sterile neutrino with a mass in a range of 0 - 1.5 GeV. The determined B+→μ+ νμB^+ \to μ^+ \, ν_μ branching fraction limit is further used to constrain the mass and coupling space of the type II and type III two-Higgs-doublet models.

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