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Canonical interpretations of the newly observed $$\Xi _c(2923)^0$$ Ξ c ( 2923 ) 0 , $$\Xi _c(2939)^0$$ Ξ c ( 2939 ) 0 , and $$\Xi _c(2965)^0$$ Ξ c ( 2965 ) 0 resonances
The European Physical Journal C ( IF 4.4 ) Pub Date : 2020-10-06 , DOI: 10.1140/epjc/s10052-020-08488-5
Qi-Fang Lü

Three neutral resonances \(\Xi _c(2923)^0\), \(\Xi _c(2939)^0\), and \(\Xi _c(2965)^0\) have been observed in the \(\Lambda _c^+ K^-\) mass spectrum by the LHCb Collaboration. Given the \(\Xi _c\) and \(\Xi _c^\prime \) mass spectra predicted by the constituent quark models, these three resonances are tentatively treated as the \(\lambda \)-mode \(\Xi _c(2S)\), \(\Xi _c^\prime (2S)\), \(\Xi _c^{\prime *}(2S)\), and \(\Xi _c^\prime (1P)\) states, and their strong decay behaviors are calculated within the \(^3P_0\) model. Our results indicate that the \(\Xi _c(2923)^0\) and \(\Xi _c(2939)^0\) can be clarified into the \(J^P=3/2^-\) and \(5/2^-\) \(\Xi _c^\prime (1P)\) states respectively, and the \(\Xi _c(2965)^0\) can be regarded as the \(J^P=1/2^+\) \(\Xi _c^\prime (2S)\) state. Also, we suggest that the previous observed \(\Xi _c(2930)\) may be the overlap of two structures \(\Xi _c(2923)\) and \(\Xi _c(2939)\), and the \(\Xi _c(2970)\) should be the same state as \(\Xi _c(2965)\). Other theoretical information on the missing \(\Xi _c(2S)\), \(\Xi _c^{\prime *}(2S)\), and \(\Xi _c^\prime (1P)\) states may be helpful for future experimental searches.

A preprint version of the article is available at ArXiv.


中文翻译:

对新观察到的$$ \ Xi _c(2923)^ 0 $$(c(2923)0,$$ \ Xi _c(2939)^ 0 $$Ξc(2939)0和$$ \ Xi _c的规范解释(2965)^ 0 $$Ξc(2965)0共鸣

\ {\中观察到三个中性共振\(\ Xi _c(2923)^ 0 \)\(\ Xi _c(2939)^ 0 \)\(\ Xi _c(2965)^ 0 \)通过LHCb协作获得的λ质谱。给定由组成夸克模型预测的\(\ Xi _c \)\(\ Xi _c ^ \ prime \)质谱,这三个共振被暂时视为\(\ lambda \)-模式\(\ Xi _c (2S)\)\(\ Xi _c ^ \ prime(2S)\)\(\ Xi _c ^ {\ prime *}(2S)\)\(\ Xi _c ^ \ prime(1P)\ )状态及其强烈的衰减行为在\(^ 3P_0 \)中计算模型。我们的结果表明\(\ Xi _c(2923)^ 0 \)\(\ Xi _c(2939)^ 0 \)可以明确化为\(J ^ P = 3/2 ^-\)\ (5/2 ^-\) \(\ Xi _c ^ \ prime(1P)\)状态,而\(\ Xi _c(2965)^ 0 \)可以视为\(J ^ P = 1 / 2 ^ + \) \(\ Xi _c ^ \素数(2S)\)状态。此外,我们建议先前观察到的\(\ Xi _c(2930)\)可能是两个结构\(\ Xi _c(2923)\)\(\ Xi _c(2939)\)的重叠,并且\ (\ Xi _c(2970)\)应与\(\ Xi _c(2965)\)处于相同状态。关于失踪的其他理论信息\(\ Xi _c(2S)\)\(\ Xi _c ^ {\ prime *}(2S)\)\(\ Xi _c ^ \ prime(1P)\)状态可能对将来的实验搜索有所帮助。

该文章的预印本可从ArXiv获得。
更新日期:2020-10-07
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