Measurement of R(D)\mathcal{R}(D) and R(D∗)\mathcal{R}(D^*) with a semileptonic tagging method

preprint2019arXivOpen access
The Belle CollaborationG. CariaP. UrquijoI. AdachiH. AiharaS. Al SaidD. M. AsnerH. AtmacanT. AushevV. BabuI. BadhreesA. M. BakichP. BeheraC. BeleñoJ. BennettB. BhuyanT. BilkaJ. BiswalM. BračkoT. E. BrowderM. CampajolaD. ČervenkovP. ChangR. CheaibV. ChekelianA. ChenB. G. CheonK. ChilikinH. E. ChoK. ChoY. ChoiS. ChoudhuryD. CinabroS. CunliffeN. DashG. De NardoF. Di CapuaS. Di CarloZ. DoležalT. V. DongS. EidelmanD. EpifanovJ. E. FastT. FerberD. FerlewiczB. G. FulsomR. GargV. GaurN. GabyshevA. GarmashA. GiriP. GoldenzweigD. GreenwaldO. GrzymkowskaY. GuanO. HartbrichK. HayasakaH. HayashiiT. HiguchiW. -S. HouC. -L. HsuK. InamiG. IngugliaA. IshikawaR. ItohM. IwasakiY. IwasakiW. W. JacobsH. B. JeonS. JiaY. JinD. JoffeK. K. JooA. B. KaliyarK. H. KangG. KaryanT. KawasakiH. KichimiC. H. KimD. Y. KimH. J. KimK. T. KimS. H. KimK. KinoshitaP. KodyšS. KorparD. KotchetkovR. KroegerP. KrokovnyR. KumarY. -J. KwonJ. S. LangeI. S. LeeJ. K. LeeS. C. LeeL. K. LiY. B. LiL. Li GioiJ. LibbyK. LieretD. LiventsevT. LuoM. MasudaT. MatsudaD. MatvienkoM. MerolaF. MetznerK. MiyabayashiG. B. MohantyT. J. MoonT. MoriR. MussaK. R. NakamuraK. J. NathM. NayakN. K. NisarS. NishidaK. NishimuraK. OgawaH. OnoY. OnukiP. OskinP. PakhlovG. PakhlovaB. PalT. PangH. ParkS. -H. ParkS. PatraS. PaulT. K. PedlarR. PestotnikL. E. PiilonenV. PopovE. PrencipeM. T. PrimA. RabusovP. K. ResmiM. RitterG. RussoD. SahooS. SandilyaL. SanteljT. SanukiO. SchneiderG. SchnellJ. SchuelerC. SchwandaY. SeinoK. SenyoM. E. SeviorV. ShebalinJ. -G. ShiuB. ShwartzF. SimonA. SokolovE. SolovievaM. StaričZ. S. StottlerT. SumiyoshiW. SutcliffeM. TakizawaU. TamponiK. TanidaF. TenchiniM. UchidaT. UglovS. UnoY. UsovS. E. VahsenR. van TonderG. VarnerA. VossenE. WaheedB. WangC. H. WangM. -Z. WangP. WangX. L. WangS. WatanukiJ. WiechczynskiE. WonH. YamamotoS. B. YangH. YeJ. H. YinC. Z. YuanZ. P. ZhangV. ZhilichV. ZhukovaV. Zhulanov

Abstract

The experimental results on the ratios of branching fractions R(D)=B(Bˉ→Dτ−νˉτ)/B(Bˉ→Dℓ−νˉℓ)\mathcal{R}(D) = {\cal B}(\bar{B} \to D τ^- \barν_τ)/{\cal B}(\bar{B} \to D \ell^- \barν_{\ell}) and R(D∗)=B(Bˉ→D∗τ−νˉτ)/B(Bˉ→D∗ℓ−νˉℓ)\mathcal{R}(D^*) = {\cal B}(\bar{B} \to D^* τ^- \barν_τ)/{\cal B}(\bar{B} \to D^* \ell^- \barν_{\ell}), where ℓ\ell denotes an electron or a muon, show a long-standing discrepancy with the Standard Model predictions, and might hint to a violation of lepton flavor universality. We report a new simultaneous measurement of R(D)\mathcal{R}(D) and R(D∗)\mathcal{R}(D^*), based on a data sample containing 772×106772 \times 10^6 BBˉB\bar{B} events recorded at the Υ(4S)Υ(4S) resonance with the Belle detector at the KEKB e+e−e^+ e^- collider. In this analysis the tag-side BB meson is reconstructed in a semileptonic decay mode and the signal-side ττ is reconstructed in a purely leptonic decay. The measured values are R(D)=0.307±0.037±0.016\mathcal{R}(D)= 0.307 \pm 0.037 \pm 0.016 and R(D∗)=0.283±0.018±0.014\mathcal{R}(D^*) = 0.283 \pm 0.018 \pm 0.014, where the first uncertainties are statistical and the second are systematic. These results are in agreement with the Standard Model predictions within 0.20.2, 1.11.1 and 0.80.8 standard deviations for R(D)\mathcal{R}(D), R(D∗)\mathcal{R}(D^*) and their combination, respectively. This work constitutes the most precise measurements of R(D)\mathcal{R}(D) and R(D∗)\mathcal{R}(D^*) performed to date as well as the first result for R(D)\mathcal{R}(D) based on a semileptonic tagging method.

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