Search for tetraquark states XccsˉsˉX_{cc\bar{s}\bar{s}} in Ds+Ds+ (Ds∗+Ds∗+)D_{s}^{+}D_{s}^{+}~(D_{s}^{*+}D_{s}^{*+}) final states at Belle

preprint2022arXivOpen access
Belle CollaborationX. Y. GaoY. LiC. P. ShenI. AdachiH. AiharaD. M. AsnerH. AtmacanT. AushevR. AyadP. BeheraK. BelousM. BessnerV. BhardwajB. BhuyanT. BilkaA. BobrovD. BodrovG. BonviciniJ. BorahA. BozekM. BračkoT. E. BrowderA. BudanoM. CampajolaD. ČervenkovM. -C. ChangP. ChangA. ChenB. G. CheonK. ChilikinH. E. ChoK. ChoS. -J. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroS. CunliffeS. DasG. De PietroR. DhamijaF. Di CapuaJ. DingfelderZ. DoležalT. V. DongD. DossettT. FerberA. FreyB. G. FulsomR. GargV. GaurN. GabyshevA. GiriP. GoldenzweigT. GuY. GuanK. GudkovaC. HadjivasiliouS. HalderO. HartbrichK. HayasakaH. HayashiiM. T. HedgesW. -S. HouC. -L. HsuT. IijimaK. InamiG. IngugliaA. IshikawaR. ItohM. IwasakiY. IwasakiW. W. JacobsE. -J. JangS. JiaY. JinK. K. JooJ. KahnA. B. KaliyarK. H. KangG. KaryanT. KawasakiH. KichimiC. KieslingC. H. KimD. Y. KimK. -H. KimY. -K. KimP. KodyšT. KonnoA. KorobovS. KorparE. KovalenkoP. KrižanR. KroegerP. KrokovnyT. KuhrR. KumarK. KumaraA. KuzminY. -J. KwonY. -T. LaiT. LamJ. S. LangeM. LaurenzaS. C. LeeC. H. LiJ. LiL. K. LiY. B. LiL. Li GioiJ. LibbyK. LieretD. LiventsevA. MartiniM. MasudaT. MatsudaD. MatvienkoS. K. MauryaF. MeierM. MerolaF. MetznerK. MiyabayashiR. MizukG. B. MohantyR. MussaM. NakaoZ. NatkaniecA. NatochiiL. NayakM. NiiyamaN. K. NisarS. NishidaK. OgawaS. OgawaH. OnoP. OskinP. PakhlovG. PakhlovaT. PangS. PardiH. ParkS. -H. ParkS. PatraS. PaulT. K. PedlarR. PestotnikL. E. PiilonenT. PodobnikV. PopovE. PrencipeM. T. PrimM. RöhrkenA. RostomyanN. RoutG. RussoD. SahooS. SandilyaA. SangalL. SanteljT. SanukiV. SavinovG. SchnellY. SeinoK. SenyoM. E. SeviorM. ShapkinC. SharmaJ. -G. ShiuF. SimonJ. B. SinghA. SokolovE. SolovievaS. StaničM. StaričZ. S. StottlerM. SumihamaT. SumiyoshiM. TakizawaU. TamponiK. TanidaF. TenchiniM. UchidaK. UnoS. UnoP. UrquijoY. UsovR. van TonderG. VarnerA. VinokurovaE. WaheedE. WangM. -Z. WangX. L. WangM. WatanabeS. WatanukiE. WonX. XuB. D. YabsleyW. YanS. B. YangH. YeJ. H. YinC. Z. YuanY. ZhaiZ. P. ZhangV. ZhilichV. Zhukova

Abstract

A search for double-heavy tetraquark state candidates XccsˉsˉX_{cc\bar{s}\bar{s}} decaying to Ds+Ds+D_{s}^{+}D_{s}^{+} and Ds∗+Ds∗+D_{s}^{*+} D_{s}^{*+} is presented for the first time using the data samples of 102 million Υ(1S)Υ(1S) and 158 million Υ(2S)Υ(2S) events, and the data samples at s\sqrt{s} = 10.52~GeV, 10.58~GeV, and 10.867~GeV corresponding to integrated luminosities of 89.5~fb−1^{-1}, 711.0~fb−1^{-1}, and 121.4~fb−1^{-1}, respectively, accumulated with the Belle detector at the KEKB asymmetric energy electron-positron collider. The invariant-mass spectra of the Ds+Ds+D_{s}^{+}D_{s}^{+} and Ds∗+Ds∗+D_{s}^{*+} D_{s}^{*+} are studied to search for possible resonances. No significant signals are observed, and the 90\% confidence level upper limits on the product branching fractions [B(Υ(1S,2S)→Xccsˉsˉ+anything)×B(Xccsˉsˉ→Ds+Ds+(Ds∗+Ds∗+)){\cal B}(Υ(1S,2S) \to X_{cc\bar{s}\bar{s}} + anything) \times {\cal B}(X_{cc\bar{s}\bar{s}} \to D_{s}^{+}D_{s}^{+}(D_{s}^{*+} D_{s}^{*+}))] in Υ(1S,2S)Υ(1S,2S) inclusive decays and the product values of Born cross section and branching fraction [σ(e+e−→Xccsˉsˉ+anything)×B(Xccsˉsˉ→Ds+Ds+(Ds∗+Ds∗+))σ(e^+e^- \to X_{cc\bar{s}\bar{s}} + anything ) \times {\cal B}(X_{cc\bar{s}\bar{s}} \to D_{s}^{+}D_{s}^{+}(D_{s}^{*+} D_{s}^{*+}))] in e+e−e^+e^- collisions at s\sqrt{s} = 10.52~GeV, 10.58~GeV, and 10.867~GeV under different assumptions of XccsˉsˉX_{cc\bar{s}\bar{s}} masses and widths are obtained.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.