Baryon interactions from lattice QCD with physical masses —S = −3 sector: Ξ∑ and Ξ∑-Λ

Hyperon-nucleon and hyperon-hyperon interactions are important in studying the properties of hypernuclei in hypernuclear physics. However, unlike the nucleons which are quite stable, hyperons are unstable so that the direct scattering experiments are difficult, which leads to the large uncertainty i...

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Published inEPJ Web of Conferences Vol. 175; p. 5013
Main Authors Ishii, Noriyoshi, Aoki, Sinya, Doi, Takumi, Gongyo, Shinya, Hatsuda, Tetsuo, Ikeda, Yoichi, Inoue, Takashi, Iritani, Takumi, Miyamoto, Takaya, Nemura, Hidekatsu, Sasaki, Kenji
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LanguageEnglish
Published Les Ulis EDP Sciences 01.01.2018
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Abstract Hyperon-nucleon and hyperon-hyperon interactions are important in studying the properties of hypernuclei in hypernuclear physics. However, unlike the nucleons which are quite stable, hyperons are unstable so that the direct scattering experiments are difficult, which leads to the large uncertainty in the phenomenological determination of hyperon potentials. In this talk, we use the gauge configurations generated at the (almost) physical point ( m π = 146 MeV) on a huge spatial volume (8:1fm) 4 to present our latest result on the hyperon-hyperon potentials in S = −3 sector (Ξ∑ single channel and Ξ∑- ΞΛ; coupled channel) from the Nambu-Bethe-Salpeter wave functions based on the HAL QCD method with improved statistics.
AbstractList Hyperon-nucleon and hyperon-hyperon interactions are important in studying the properties of hypernuclei in hypernuclear physics. However, unlike the nucleons which are quite stable, hyperons are unstable so that the direct scattering experiments are difficult, which leads to the large uncertainty in the phenomenological determination of hyperon potentials. In this talk, we use the gauge configurations generated at the (almost) physical point (mπ = 146 MeV) on a huge spatial volume (8:1fm)4 to present our latest result on the hyperon-hyperon potentials in S = −3 sector (Ξ∑ single channel and Ξ∑- ΞΛ; coupled channel) from the Nambu-Bethe-Salpeter wave functions based on the HAL QCD method with improved statistics.
Hyperon-nucleon and hyperon-hyperon interactions are important in studying the properties of hypernuclei in hypernuclear physics. However, unlike the nucleons which are quite stable, hyperons are unstable so that the direct scattering experiments are difficult, which leads to the large uncertainty in the phenomenological determination of hyperon potentials. In this talk, we use the gauge configurations generated at the (almost) physical point ( m π = 146 MeV) on a huge spatial volume (8:1fm) 4 to present our latest result on the hyperon-hyperon potentials in S = −3 sector (Ξ∑ single channel and Ξ∑- ΞΛ; coupled channel) from the Nambu-Bethe-Salpeter wave functions based on the HAL QCD method with improved statistics.
Author Doi, Takumi
Ishii, Noriyoshi
Miyamoto, Takaya
Ikeda, Yoichi
Iritani, Takumi
Gongyo, Shinya
Sasaki, Kenji
Nemura, Hidekatsu
Inoue, Takashi
Aoki, Sinya
Hatsuda, Tetsuo
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CitedBy_id crossref_primary_10_1088_1674_1137_ac988a
crossref_primary_10_1103_PhysRevC_105_035203
crossref_primary_10_1007_s00601_024_01908_2
crossref_primary_10_1007_s00601_021_01685_2
crossref_primary_10_1016_j_physletb_2022_137223
crossref_primary_10_1103_PhysRevC_108_055201
crossref_primary_10_1103_PhysRevC_103_025201
crossref_primary_10_1088_1742_6596_1643_1_012171
Cites_doi 10.1143/PTP.123.89
10.1103/PhysRevLett.99.022001
10.1016/j.physletb.2012.04.076
10.2183/pjab.87.509
10.1016/j.nuclphysa.2012.02.008
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SubjectTerms Hypernuclei
Hyperons
Nucleons
Quantum chromodynamics
Wave functions
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Title Baryon interactions from lattice QCD with physical masses —S = −3 sector: Ξ∑ and Ξ∑-Λ
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