Search for gamma (1S,2S) -> Z(c)(+)Z(c)((')-) and e(+)e(-) -> Z(c)(+)Z(c)((')-) at root s=10.52, 10.58, and 10.867 Gev
Search for gamma (1S,2S) -> Z(c)(+)Z(c)((')-) and e(+)e(-) -> Z(c)(+)Z(c)((')-) at root s=10.52, 10.58, and 10.867 Gev
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DOI:
10.1103/physrevd.97.112004
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发表时间:
2018
影响因子:
5
通讯作者:
K
中科院分区:
文献类型:
--
作者:
Jia S.;Shen C. P.;Yuan;C. Z.;Adachi;I.;Aihara;H.;Al Said;S.;Asner;D. M.;Aulchenko;V.;Aushev;T.;Ayad;R.;Baba;V.;Badhrees;I.;Bansa;V.;Behera;P.;Beleno;C.;Bhuyan;B.;Bilka;T.;Biswa;J.;Bozek;A.;Bracko;M.;Cervenkov;D.;Chekelian;V.;Chen;A.;Cheon;B. G.;Chilikin;K
The first search for double charged charmoniumlike state production in ϒ(1S) and ϒ(2S) decays and inannihilation at, 10.58, and 10.867 GeV is conducted using data collected with the Belle detector at the KEKB asymmetric energy electron-positron collider. No significant signals are observed in any of the studied modes, and the 90% credibility level upper limits on their product branching fractions in ϒ(1S) and ϒ(2S) decays [B(ϒ(1S,2S)→Zc+Zc(′)-)×B(Zc+→π++cc¯) (,,)] and the product of Born cross section and branching fraction for() at, 10.58, and 10.867 GeV are determined. Here,refers to theandobserved in thefinal state, theandin thefinal state, and theandin thefinal state.