検索対象:     
報告書番号:
※ 半角英数字
 年 ~ 
 年
検索結果: 4 件中 1件目~4件目を表示
  • 1

発表形式

Initialising ...

選択項目を絞り込む

掲載資料名

Initialising ...

発表会議名

Initialising ...

筆頭著者名

Initialising ...

キーワード

Initialising ...

発表言語

Initialising ...

発行年

Initialising ...

開催年

Initialising ...

選択した検索結果をダウンロード

論文

Improved prediction of the mass splitting for $$P$$-wave $$Omega$$ baryons

Su, N.*; Chen, H.-X.*; Gubler, P.; 保坂 淳

Physical Review D, 113(1), p.016005_1 - 016005_7, 2026/01

 被引用回数:1 パーセンタイル:67.85(Astronomy & Astrophysics)

Using the QCD sum rule method, we investigate the mass splitting for the spin-orbit partner states of the $$Omega(2012)$$ baryon assuming that it is a $$P$$-wave excitation with $$J^P = 3/2^-$$. This study is an extension of a previous work, in which the masses of these states were estimated with uncertainties too large to extract the reliable mass splitting. In the present study, by directly formulating a sum rule for the mass splitting, we obtain an improved prediction, $$delta M = M_{3/2^-} - M_{1/2^-} = -18.0^{+33.6}_{-17.1}$$ MeV. This result provides a more quantitative insight into the spectrum of $$P$$-wave $$Omega$$ baryons and serves as a useful reference for future experiments.

論文

Investigation on the $$Omega(2012)$$ from QCD sum rules

Su, N.*; Chen, H.-X.*; Gubler, P.; 保坂 淳

Proceedings of Science (Internet), 500, p.076_1 - 076_6, 2026/01

We investigate the recently observed $$Omega(2012)$$ baryon using QCD sum rules. By constructing P-wave $$Omega$$ baryon currents and performing spin projection and parity projection, we obtain the masses of the $$J^P = 1/2^{-}$$ and $$3/2^{-}$$ states as $$M_{1/2^-} = 2.07^{+0.07}_{-0.07}$$ GeV and $$M_{3/2^-} = 2.05^{+0.09}_{-0.10}$$ GeV, in good agreement with experiment. This suggests that $$Omega(2012)$$ is likely to be a negative parity P-wave excited state, though its spin remains undetermined and requires further study of its decay properties.

論文

Investigation on the $$Omega(2012)$$ from QCD sum rules

Su, N.*; Chen, H.-X.*; Gubler, P.; 保坂 淳

Nuclear and Particle Physics Proceedings, 347, p.2 - 5, 2024/12

We investigate the recently observed $$Omega(2012)$$ baryon using QCD sum rules. By constructing P-wave $$Omega$$ baryon currents and performing spin projection and parity projection, we obtain the masses of the $$J^P = 1/2^{-}$$ and $$3/2^{-}$$ states as $$M_{1/2^-} = 2.07^{+0.07}_{-0.07}$$ GeV and $$M_{3/2^-} = 2.05^{+0.09}_{-0.10}$$ GeV, in good agreement with experiment. This suggests that $$Omega(2012)$$ is likely to be a negative parity P-wave excited state, though its spin remains undetermined and requires further study of its decay properties.

論文

Investigation on the $$Omega(2012)$$ from QCD sum rules

Su, N.*; Chen, H.-X.*; Gubler, P.; 保坂 淳

Physical Review D, 110(3), p.034007_1 - 034007_9, 2024/08

 被引用回数:9 パーセンタイル:70.13(Astronomy & Astrophysics)

We study the recently observed $$Omega(2012)$$ baryon in quantum chromodynamics (QCD) sum rules. We construct the P-wave $$Omega$$ baryon currents with a covariant derivative, and perform spin projection to obtain the currents with total spin 1/2 and 3/2. We then apply the parity-projected QCD sum rules to separate the contributions of the positive and negative parity states. We extract the masses of $$J^P = 1/2^{-}$$ and $$3/2^{-}$$ states to be $$M_{1/2^-} = 2.07^{+0.07}_{-0.07}$$ GeV and $$M_{3/2^-} = 2.05^{+0.09}_{-0.10}$$ GeV. Both results are in good agreement with the experimental result. Therefore, it is likely that the $$Omega(2012)$$ is a negative parity state, which is interpreted as a P-wave excited state in the quark model. However, its spin is not determined in the present analysis, which can be done by detailed study on its decay properties.

4 件中 1件目~4件目を表示
  • 1