scholarly journals Charmed baryon weak decays with SU(3) flavor symmetry

2017 ◽  
Vol 2017 (11) ◽  
Author(s):  
C. Q. Geng ◽  
Y. K. Hsiao ◽  
Chia-Wei Liu ◽  
Tien-Hsueh Tsai
Keyword(s):  
Flavor Symmetry ◽  
Charmed Baryon ◽  
Weak Decays

scholarly journals Charmed baryon weak decays with decuplet baryon and SU(3) flavor symmetry

2019 ◽  
Vol 99 (11) ◽  
Author(s):  
Chao-Qiang Geng ◽  
Chia-Wei Liu ◽  
Tien-Hsueh Tsai ◽  
Yao Yu
Keyword(s):  
Flavor Symmetry ◽  
Charmed Baryon ◽  
Weak Decays ◽  
Decuplet Baryon

scholarly journals Charmed baryon decay to a strange baryon plus a pion using QCD sum rules

2019 ◽  
Vol 34 (03n04) ◽  
pp. 1950015 ◽  
Author(s):  
Leonard S. Kisslinger ◽  
Bijit Singha
Keyword(s):  
Sum Rules ◽  
Qcd Sum Rules ◽  
Charmed Baryons ◽  
Charmed Baryon ◽  
Strange Baryon ◽  
Weak Decays ◽  
Baryon Decay

This is an extension of the prediction of strange baryon decays to the decays of charmed baryons using QCD sum rules. Using QCD sum rules, we estimate the decay [Formula: see text]. Although some weak decays of the [Formula: see text] have been measured, since it is difficult to measure [Formula: see text] our estimates should be useful for future experiments.

scholarly journals Charmed baryon spectroscopy and light flavor symmetry from lattice QCD

2015 ◽  
Vol 92 (3) ◽  
Author(s):  
Paula Pérez-Rubio ◽  
Sara Collins ◽  
Gunnar S. Bali
Keyword(s):  
Lattice Qcd ◽  
Flavor Symmetry ◽  
Charmed Baryon ◽  
Baryon Spectroscopy

scholarly journals Hadronic weak decays of the charmed baryon Ωc

2020 ◽  
Vol 101 (9) ◽  
Author(s):  
Shiyong Hu ◽  
Guanbao Meng ◽  
Fanrong Xu
Keyword(s):  
Charmed Baryon ◽  
Weak Decays

Charmed-baryon weak decays in heavy-quark effective theory

1992 ◽  
Vol 45 (9) ◽  
pp. R3024-R3026 ◽  
Author(s):  
Gurpreet Kaur ◽  
M. P. Khanna
Keyword(s):  
Heavy Quark ◽  
Effective Theory ◽  
Heavy Quark Effective Theory ◽  
Charmed Baryon ◽  
Weak Decays

scholarly journals Doubly charmed tetraquarks in a diquark–antidiquark model

2018 ◽  
Vol 33 (16) ◽  
pp. 1850096 ◽  
Author(s):  
Xiaojun Yan ◽  
Bin Zhong ◽  
Ruilin Zhu
Keyword(s):  
Excited States ◽  
Flavor Symmetry ◽  
Tetraquark State ◽  
Charmed Mesons ◽  
Charmed Baryon ◽  
Light Baryon ◽  
State Formula

We study the spectra of the doubly charmed tetraquark states in a diquark–antidiquark model. The doubly charmed tetraquark states form an antitriplet and sextet configurations according to flavor SU(3) symmetry. For the tetraquark state [Formula: see text], we show the mass for both bound and excited states. The two-body decays of tetraquark states [Formula: see text] and [Formula: see text] to charmed mesons have also been studied. In the end, the doubly charmed tetraquarks decays to a charmed baryon and a light baryon have been studied in the SU(3) flavor symmetry.

scholarly journals Three-body charmed baryon decays with SU(3) flavor symmetry

2019 ◽  
Vol 99 (7) ◽  
Author(s):  
C. Q. Geng ◽  
Y. K. Hsiao ◽  
Chia-Wei Liu ◽  
Tien-Hsueh Tsai
Keyword(s):  
Flavor Symmetry ◽  
Charmed Baryon ◽  
Three Body

scholarly journals Two-body charmed baryon decays involving decuplet baryon in the quark-diagram scheme

2020 ◽  
Vol 80 (11) ◽  
Author(s):  
Y. K. Hsiao ◽  
Qian Yi ◽  
Shu-Ting Cai ◽  
H. J. Zhao
Keyword(s):  
Pseudoscalar Meson ◽  
Branching Fractions ◽  
Flavor Symmetry ◽  
Isospin Symmetry ◽  
Charmed Baryon ◽  
Decay Channels ◽  
Decuplet Baryon ◽  
Exchange Processes ◽  
Quark Diagram ◽  
Cabibbo Suppressed

AbstractIn the quark-diagram scheme, we study the charmed baryon decays of $$\mathbf{B}_c\rightarrow \mathbf{B}^* M$$ B c → B ∗ M , where $$\mathbf{B}_c$$ B c is $$\Lambda _c^+$$ Λ c + or $$\Xi _c^{+(0)}$$ Ξ c + ( 0 ) , together with $$\mathbf{B}^*$$ B ∗ (M) the decuplet baryon (pseudoscalar meson). It is found that only two W-exchange processes are allowed to contribute to $$\mathbf{B}_c\rightarrow \mathbf{B}^* M$$ B c → B ∗ M . Particularly, we predict $${\mathcal {B}}(\Lambda _c^+ \rightarrow \Sigma ^{*0(+)} \pi ^{+(0)})=(2.8\pm 0.4)\times 10^{-3}$$ B ( Λ c + → Σ ∗ 0 ( + ) π + ( 0 ) ) = ( 2.8 ± 0.4 ) × 10 - 3 , which respects the isospin symmetry. Besides, we take into account the SU(3) flavor symmetry breaking, in order to explain the observation of $${\mathcal {B}}(\Lambda _c^+\rightarrow \Sigma ^{*+}\eta )$$ B ( Λ c + → Σ ∗ + η ) . For the decays involving $$\Delta ^{++}(uuu)$$ Δ + + ( u u u ) , we predict $${\mathcal {B}}(\Lambda _c^+\rightarrow \Delta ^{++} \pi ^-,\Xi _c^+ \rightarrow \Delta ^{++} K^-) =(7.0\pm 1.4,13.5\pm 2.7)\times 10^{-4}$$ B ( Λ c + → Δ + + π - , Ξ c + → Δ + + K - ) = ( 7.0 ± 1.4 , 13.5 ± 2.7 ) × 10 - 4 as the largest branching fractions in the singly Cabibbo-suppressed $$\Lambda _c^+,\Xi _c^+\rightarrow \mathbf{B}^*M$$ Λ c + , Ξ c + → B ∗ M decay channels, respectively, which are accessible to the LHCb, BELLEII and BESIII experiments.

Two-body charmed-baryon weak decays

1991 ◽  
Vol 44 (1) ◽  
pp. 182-185 ◽  
Author(s):  
Gurpreet Kaur ◽  
M. P. Khanna
Keyword(s):  
Charmed Baryon ◽  
Weak Decays
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