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《中国物理C》（英文）编辑部
2024年10月30日
Chinese Physics C> 2018, Vol. 42> Issue(1) : 014105 DOI: 10.1088/1674-1137/42/1/014105

Leading order relativistic hyperon-nucleon interactions in chiral effective field theory

  • 1.

      School of Physics and Nuclear Energy Engineering and International Research Center for Nuclei and Particles in the Cosmos, Beihang University, Beijing 100191, China

  • 2.

      School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China

  • 3.

     School of Physics and Nuclear Energy Engineering and International Research Center for Nuclei and Particles in the Cosmos, Beihang University, Beijing 100191, China

  • 4.

     Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University, Beijing 100191, China

  • 5.

      Center for Theoretical Physics, Department of Physics, Sichuan University, 29 Wang-Jiang Road, Chengdu, Sichuan 610064, China

  • We apply a recently proposed covariant power counting in nucleon-nucleon interactions to study strangeness S=-1 ΛN-∑N interactions in chiral effective field theory. At leading order, Lorentz invariance introduces 12 low energy constants, in contrast to the heavy baryon approach, where only five appear. The Kadyshevsky equation is adopted to resum the potential in order to account for the non-perturbative nature of hyperon-nucleon interactions. A fit to the 36 hyperon-nucleon scattering data points yields χ2≈ 16, which is comparable with the sophisticated phenomenological models and the next-to-leading order heavy baryon approach. However, one cannot achieve a simultaneous description of the nucleon-nucleon phase shifts and strangeness S=-1 hyperon-nucleon scattering data at leading order.
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Kai-Wen Li, Xiu-Lei Ren, Li-Sheng Geng and Bing-Wei Long. Leading order relativistic hyperon-nucleon interactions in chiral effective field theory[J]. Chinese Physics C, 2018, 42(1): 014105. doi: 10.1088/1674-1137/42/1/014105
Kai-Wen Li, Xiu-Lei Ren, Li-Sheng Geng and Bing-Wei Long. Leading order relativistic hyperon-nucleon interactions in chiral effective field theory[J]. Chinese Physics C, 2018, 42(1): 014105.  doi: 10.1088/1674-1137/42/1/014105 shu
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Received: 2017-07-15
Revised: 2017-10-25
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    Supported by the National Natural Science Foundation of China (11375024, 11522539, 11375120), the China Postdoctoral Science Foundation (2016M600845, 2017T100008) and the Fundamental Research Funds for the Central Universities

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Leading order relativistic hyperon-nucleon interactions in chiral effective field theory

    Corresponding author: Li-Sheng Geng,
  • 1.  School of Physics and Nuclear Energy Engineering and International Research Center for Nuclei and Particles in the Cosmos, Beihang University, Beijing 100191, China
  • 2.  School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China
  • 3. School of Physics and Nuclear Energy Engineering and International Research Center for Nuclei and Particles in the Cosmos, Beihang University, Beijing 100191, China
  • 4. Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University, Beijing 100191, China
  • 5.  Center for Theoretical Physics, Department of Physics, Sichuan University, 29 Wang-Jiang Road, Chengdu, Sichuan 610064, China
  • Received Date: 2017-07-15
  • Accepted Date: 2017-10-25
  • Available Online: 2018-01-05
Fund Project:  Supported by the National Natural Science Foundation of China (11375024, 11522539, 11375120), the China Postdoctoral Science Foundation (2016M600845, 2017T100008) and the Fundamental Research Funds for the Central Universities

Abstract: We apply a recently proposed covariant power counting in nucleon-nucleon interactions to study strangeness S=-1 ΛN-∑N interactions in chiral effective field theory. At leading order, Lorentz invariance introduces 12 low energy constants, in contrast to the heavy baryon approach, where only five appear. The Kadyshevsky equation is adopted to resum the potential in order to account for the non-perturbative nature of hyperon-nucleon interactions. A fit to the 36 hyperon-nucleon scattering data points yields χ2≈ 16, which is comparable with the sophisticated phenomenological models and the next-to-leading order heavy baryon approach. However, one cannot achieve a simultaneous description of the nucleon-nucleon phase shifts and strangeness S=-1 hyperon-nucleon scattering data at leading order.

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