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Identifying the $$Xi_{b}(6227)$$ and $$Sigma_{b}(6097)$$ as $$P$$-wave bottom baryons of $$J^P = 3/2^-$$

P-波$$J^P=3/2^-$$状態としての$$Xi_{b}(6227)$$, $$Sigma_{b}(6097)$$粒子

Cui, E.-L.*; Yang, H.-M.*; Chen, H.-X.*; 保坂 淳

Cui, E.-L.*; Yang, H.-M.*; Chen, H.-X.*; Hosaka, Atsushi

We use the method of QCD sum rules within the framework of heavy quark effective theory to study the mass spectrum of the $$Sigma_b(6097)^{pm}$$ and $$Xi_b(6227)^-$$, and use the method of light cone sum rules still within the heavy quark effective theory to study their decay properties. Our results suggest that they can be well interpreted as $$P$$-wave bottom baryons with the spin-parity $$J^P=3/2^-$$. They belong to the baryon doublet $$[6_F,2,1,lambda]$$, where the total and spin angular momenta of the light degree of freedom are $$j_l=2$$ and $$s_l=1$$, and the orbital angular momentum is between the bottom quark and the two-light-quark system ($$lambda$$-type). This doublet contains six bottom baryons, and we predict masses (mass differences) and decay widths of the other four states to be $$M_{Omega_b(3/2^-)}=6.46pm 0.12$$ GeV, $$Gamma_{Omega_b(3/2^-)}=58^{+65}_{-33}$$ MeV, $$M_{Sigma_b(5/2^-)}-M_{Sigma_b(3/2^-)}=13pm 5$$ MeV, $$M_{Xi_b(5/2^-)}-M_{Xi_b(3/2^-)}=12pm 5$$ MeV, $$M_{Omega_b(5/2^-)}-M_{Omega_b(3/2^-)}=11pm 5$$ MeV. We propose to search for them in further LHCb experiments.

使用言語

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English

掲載資料名

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Physical Review D

巻

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99

号

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9

ページ数

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p.094021_1 - 094021_15

発行年月

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2019/05

発表会議名

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開催年月

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開催都市

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開催国

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キーワード

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no keyword

特許データ

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PDF

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論文URL

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https://doi.org/10.1103/PhysRevD.99.094021

研究データの公開先DOI

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使用施設

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広報プレスリリース

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論文解説記事
(成果普及情報誌)

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受委託・共同研究相手機関

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Access

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- Accesses

InCites™

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パーセンタイル：86.82

分野：Astronomy & Astrophysics

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