Evidence of a new excited charmed baryon decaying to Σc(2455)0,++π±Σ_{c}(2455)^{0,++} π^{\pm}

preprint2022arXivOpen access
Belle CollaborationY. B. LiC. P. ShenI. AdachiH. AiharaD. M. AsnerH. AtmacanT. AushevR. AyadV. BabuS. BahinipatiP. BeheraK. BelousJ. BennettM. BessnerV. BhardwajB. BhuyanT. BilkaD. BodrovJ. BorahA. BozekM. BračkoP. BranchiniT. E. BrowderA. BudanoM. CampajolaD. ČervenkovM. -C. ChangP. ChangB. G. CheonK. ChilikinH. E. ChoK. ChoS. -J. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroS. DasG. De PietroR. DhamijaF. Di CapuaJ. DingfelderZ. DoležalT. V. DongD. DossettD. EpifanovB. G. FulsomR. GargV. GaurA. GarmashA. GiriP. GoldenzweigE. GrazianiT. GuY. GuanK. GudkovaC. HadjivasiliouK. HayasakaH. HayashiiW. -S. HouC. -L. HsuT. IijimaK. InamiN. IpsitaA. IshikawaR. ItohM. IwasakiY. IwasakiW. W. JacobsE. -J. JangQ. P. JiS. JiaY. JinK. K. JooG. KaryanT. KawasakiH. KichimiC. KieslingC. H. KimD. Y. KimK. -H. KimY. -K. KimH. KindoK. KinoshitaP. KodyšT. KonnoA. KorobovS. KorparE. KovalenkoP. KrižanP. KrokovnyM. KumarR. KumarK. KumaraY. -J. KwonT. LamJ. S. LangeM. LaurenzaS. C. LeeC. H. LiJ. LiL. K. LiY. LiL. Li GioiJ. LibbyK. LieretD. LiventsevM. MasudaT. MatsudaD. MatvienkoS. K. MauryaF. MeierM. MerolaF. MetznerK. MiyabayashiR. MizukG. B. MohantyI. NakamuraM. NakaoZ. NatkaniecA. NatochiiL. NayakM. NiiyamaN. K. NisarS. NishidaS. OgawaH. OnoP. OskinP. PakhlovG. PakhlovaS. PardiH. ParkS. -H. ParkS. PatraS. PaulT. K. PedlarR. PestotnikL. E. PiilonenT. PodobnikE. PrencipeM. T. PrimN. RoutG. RussoS. SandilyaL. SanteljV. SavinovG. SchnellJ. SchuelerC. SchwandaY. SeinoK. SenyoM. E. SeviorM. ShapkinC. SharmaJ. -G. ShiuJ. B. SinghA. SokolovE. SolovievaM. StaričZ. S. StottlerM. SumihamaT. SumiyoshiW. SutcliffeM. TakizawaU. TamponiK. TanidaF. TenchiniK. TrabelsiT. TsuboyamaM. UchidaT. UglovY. UnnoS. UnoY. UsovR. van TonderG. VarnerK. E. VarvellE. WaheedE. WangM. -Z. WangM. WatanabeS. WatanukiO. WerbyckaJ. WiechczynskiE. WonB. D. YabsleyW. YanS. B. YangJ. YeltonJ. H. YinC. Z. YuanY. YusaY. ZhaiZ. P. ZhangV. ZhilichV. Zhukova

Abstract

We present the study of Bˉ0→Σc(2455)0,++π±pˉ\bar{B}^{0} \to Σ_{c}(2455)^{0,++} π^{\pm} \bar{p} decays based on 772×106772\times 10^{6} BBˉB\bar{B} events collected with the Belle detector at the KEKB asymmetric-energy e+e−e^+e^- collider. The Σc(2455)0,++Σ_{c}(2455)^{0,++} candidates are reconstructed via their decay to Λc+π∓Λ_{c}^{+} π^{\mp} and Λc+Λ_{c}^{+} decays to pK−π+, pKS0,pK^{-}π^{+},~pK_{S}^{0}, and Λπ+Λπ^{+} final states. The corresponding branching fractions are measured to be B(Bˉ0→Σc(2455)0π+pˉ)=(1.09±0.06±0.07)×10−4{\cal B}(\bar{B}^{0} \to Σ_{c}(2455)^{0} π^{+} \bar{p}) = (1.09 \pm 0.06 \pm 0.07)\times10^{-4} and B(Bˉ0→Σc(2455)++π−pˉ)=(1.84±0.11±0.12)×10−4{\cal B}(\bar{B}^{0} \to Σ_{c}(2455)^{++} π^{-} \bar{p}) = (1.84\pm 0.11 \pm 0.12)\times 10^{-4}, which are consistent with the world average values with improved precision. A new structure is found in the MΣc(2455)0,++π±M_{Σ_{c}(2455)^{0,++}π^{\pm}} spectrum with a significance of 4.2σ4.2σ including systematic uncertainty. The structure is possibly an excited Λc+Λ_{c}^{+} and is tentatively named Λc(2910)+Λ_{c}(2910)^{+}. Its mass and width are measured to be (2913.8±5.6±3.8)(2913.8 \pm 5.6 \pm 3.8) MeV/c2c^{2} and (51.8±20.0±18.8)(51.8\pm20.0 \pm 18.8) MeV, respectively. The products of branching fractions for the Λc(2910)+Λ_{c}(2910)^{+} are measured to be B(Bˉ0→Λc(2910)+pˉ)×B(Λc(2910)+→Σc(2455)0π+)=(9.5±3.6±1.6)×10−6{\cal B}(\bar{B}^{0} \to Λ_{c}(2910)^{+}\bar{p})\times{\cal B}(Λ_{c}(2910)^{+} \to Σ_{c}(2455)^{0}π^{+}) = (9.5 \pm 3.6 \pm 1.6)\times 10^{-6} and B(Bˉ0→Λc(2910)+pˉ)×B(Λc(2910)+→Σc(2455)++π−)=(1.24±0.35±0.10)×10−5{\cal B}(\bar{B}^{0} \to Λ_{c} (2910)^{+}\bar{p})\times {\cal B}(Λ_{c}(2910)^{+} \to Σ_{c}(2455)^{++}π^{-}) = (1.24 \pm 0.35 \pm 0.10)\times 10^{-5}. Here, the first and second uncertainties are statistical and systematic, respectively.

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