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首页> 外文期刊>International journal of modern physics, E. Nuclear physics >Discrepancy of in-medium nucleon-nucleon cross-section in different T-matrix representations
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Discrepancy of in-medium nucleon-nucleon cross-section in different T-matrix representations

机译:不同T矩阵表示形式的中等核仁-核仁横截面差异

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In this paper, we study the in-medium nucleon-nucleon (NN) cross-section by using the Dirac-Breuckner-Hartree-Fock approximation (DBHF) with T-matrix project technique for determining the nucleon self-energy. By solving Thompson equation for different partial-wave states separately, we find that the discrepancies of nucleon self-energies in various T-matrix project representations are dominated by the channels with smaller angular momentum. Although the cross-section is independent on the project of T-matrix, the medium suppression of the cross-section in various T-matrix representations are apparently different due to the self-consistency of DBHF calculation involving effect mass of nucleon as an iterative parameter. Our results also show that the cross-sections in the complete pseudovector (CPV) choices are larger than those obtained with both DBHF in the pseudoscalar (PS) choice and nonrelativistic Brueckner-Hartree-Fock with three-body force (BHF + 3BF), respectively. Further comparison shows that the neutron-proton (NP) cross-section within DBHF + PV approach, σ_(NP)~(PV), is approximately equal to and slightly larger than that evaluated with BHF + 3BF, σ_(NP)~(3BF), while the neutron-neutron (NN) (or proton-proton (PP)) cross-section given by DBHF + PV method, σ_(NN)~(PV), being the closest to the cross-section calculated by using BHF without 3BF in the lower energy region. Additionally, the discrepancies of the in-medium nucleon-nucleon differential cross-section induced by different representations of T-matrix in DBHF are discussed for nuclear matter with different densities.
机译:在本文中,我们使用Dirac-Breuckner-Hartree-Fock近似(DBHF)和T矩阵投影技术研究核内自能量,从而研究了中等核子内核(NN)的截面。通过分别针对不同的分波状态求解汤普森方程,我们发现,各种T矩阵投影表示中的核子自能差异主要由角动量较小的通道决定。尽管横截面与T矩阵的方案无关,但是由于DBHF计算的自洽性(涉及核子的有效质量作为迭代参数),因此在各种T矩阵表示形式中,横截面的介质抑制显然有所不同。 。我们的结果还表明,完全伪向量(CPV)选择中的横截面大于伪标量(PS)选择中的DBHF和三体力(BHF + 3BF)的非相对论性Brueckner-Hartree-Fock所获得的横截面,分别。进一步的比较表明,DBHF + PV方法中的中子-质子(NP)截面σ_(NP)〜(PV)大约等于并且稍大于BHF + 3BFσ_(NP)〜( 3BF),而DBHF + PV方法给出的中子-中子(NN)(或质子-质子(PP))截面为σ_(NN)〜(PV),最接近于使用在较低能量区域中没有3BF的BHF。此外,对于不同密度的核物质,还讨论了由DBHF中T矩阵的不同表示引起的中等核子-核子差异截面的差异。

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