Search for a light Higgs boson in single-photon decays of Υ(1S)Υ(1S) using Υ(2S)→π+π−Υ(1S)Υ(2S) \to π^+ π^- Υ(1S) tagging method

preprint2022arXivOpen access
Belle CollaborationS. JiaC. P. ShenI. AdachiH. AiharaS. Al SaidD. M. AsnerH. AtmacanT. AushevR. AyadV. BabuP. BeheraK. BelousJ. BennettM. BessnerV. BhardwajB. BhuyanT. BilkaA. BobrovD. BodrovG. BonviciniJ. BorahM. BračkoP. BranchiniT. E. BrowderA. BudanoM. CampajolaD. ČervenkovM. -C. ChangP. ChangV. ChekelianA. ChenB. G. CheonK. ChilikinH. E. ChoK. ChoS. -J. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroS. CunliffeS. DasN. DashG. De NardoG. De PietroR. DhamijaF. Di CapuaZ. DoležalT. V. DongD. EpifanovT. FerberD. FerlewiczB. G. FulsomR. GargV. GaurN. GabyshevA. GiriP. GoldenzweigB. GolobE. GrazianiY. GuanK. GudkovaC. HadjivasiliouT. HaraK. HayasakaH. HayashiiM. T. HedgesW. -S. HouK. InamiG. IngugliaA. IshikawaR. ItohM. IwasakiY. IwasakiW. W. JacobsE. -J. JangY. JinK. K. JooJ. KahnA. B. KaliyarK. H. KangT. KawasakiC. KieslingC. H. KimD. Y. KimK. -H. KimY. -K. KimK. KinoshitaP. KodyšS. KohaniT. KonnoA. KorobovS. KorparE. KovalenkoP. KrižanR. KroegerP. KrokovnyM. KumarR. KumarK. KumaraY. -J. KwonT. LamM. LaurenzaS. C. LeeJ. LiL. K. LiY. LiY. B. LiL. Li GioiJ. LibbyK. LieretD. LiventsevA. MartiniM. MasudaT. MatsudaD. MatvienkoS. K. MauryaF. MeierM. MerolaF. MetznerK. MiyabayashiR. MizukG. B. MohantyM. NakaoD. NarwalZ. NatkaniecA. NatochiiL. NayakN. K. NisarS. NishidaK. NishimuraK. OgawaS. OgawaH. OnoP. OskinP. PakhlovG. PakhlovaT. PangS. PardiS. -H. ParkS. PatraS. PaulT. K. PedlarR. PestotnikL. E. PiilonenT. PodobnikE. PrencipeM. T. PrimM. RöhrkenA. RostomyanN. RoutG. RussoD. SahooS. SandilyaA. SangalL. SanteljT. SanukiV. SavinovG. SchnellJ. SchuelerC. SchwandaY. SeinoK. SenyoM. E. SeviorM. ShapkinC. SharmaV. ShebalinJ. -G. ShiuB. ShwartzJ. B. SinghA. SokolovE. SolovievaS. StaničM. StaričZ. S. StottlerM. SumihamaK. SumisawaT. SumiyoshiW. SutcliffeM. TakizawaU. TamponiK. TanidaF. TenchiniK. TrabelsiM. UchidaS. UeharaT. UglovY. UnnoK. UnoS. UnoP. UrquijoS. E. VahsenR. van TonderG. VarnerA. VinokurovaE. WaheedD. WangE. WangM. -Z. WangS. WatanukiE. WonB. D. YabsleyW. YanS. B. YangH. YeJ. YeltonJ. H. YinY. YusaY. ZhaiZ. P. ZhangV. ZhilichV. Zhukova

Abstract

We search for a light Higgs boson (A0A^0) decaying into a τ+τ−τ^+τ^- or μ+μ−μ^+μ^- pair in the radiative decays of Υ(1S)Υ(1S). The production of Υ(1S)Υ(1S) mesons is tagged by Υ(2S)→π+π−Υ(1S)Υ(2S)\to π^+ π^- Υ(1S) transitions, using 158 million Υ(2S)Υ(2S) events accumulated with the Belle detector at the KEKB asymmetric energy electron-positron collider. No significant A0A^0 signals in the mass range from the τ+τ−τ^+τ^- or μ+μ−μ^+μ^- threshold to 9.2 GeV/c2c^2 are observed. We set the upper limits at 90\% credibility level (C.L.) on the product branching fractions for Υ(1S)→γA0Υ(1S)\to γA^0 and A0→τ+τ−A^0\to τ^+τ^- varying from 3.8×10−63.8\times10^{-6} to 1.5×10−41.5\times10^{-4}. Our results represent an approximately twofold improvement on the current world best upper limits for the Υ(1S)→γA0(→τ+τ−)Υ(1S)\to γA^0(\to τ^+τ^-) production. For A0→μ+μ−A^0\to μ^+μ^-, the upper limits on the product branching fractions for Υ(1S)→γA0Υ(1S)\to γA^0 and A0→μ+μ−A^0\to μ^+μ^- are at the same level as the world average limits, and vary from 3.1×10−73.1\times10^{-7} to 1.6×10−51.6\times10^{-5}. The upper limits at 90\% C.L. on the Yukawa coupling fΥ(1S)f_{Υ(1S)} and mixing angle sinθA0{\rm sin}θ_{A^0} are also given.

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