2013
DOI: 10.1103/physrevc.87.015204
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Nuclear symmetry energy from QCD sum rules

Abstract: We calculate the nucleon self-energies in isospin-asymmetric nuclear matter using QCD sum rules. Taking the difference of these for the neutron and proton enables us to express the potential part of the nuclear symmetry energy in terms of local operators. We find that the scalar (vector) self energy part gives a negative (positive) contribution to the nuclear symmetry energy which is consistent with the results from relativistic mean field theories. Moreover, we find that an important contribution to the negat… Show more

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Cited by 16 publications
(34 citation statements)
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“…where we have q 2 0 = (q · u) 2 , u = (1, 0), and c 1 = 7t 2 − 2t − 5, c 2 = 1 − t 2 , c 3 = 2t 2 − 2t − 1, c 4 = 5t 2 + 2t + 5 and c 5 = 7t 2 + 10t + 7 [89]. In this work, the following condensates are included for the QCDSR equations, Now we generalize the above results of SNM to the case of ANM, and the QCDSR equations for the proton are given by [95],…”
Section: Ope Coefficientsmentioning
confidence: 95%
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“…where we have q 2 0 = (q · u) 2 , u = (1, 0), and c 1 = 7t 2 − 2t − 5, c 2 = 1 − t 2 , c 3 = 2t 2 − 2t − 1, c 4 = 5t 2 + 2t + 5 and c 5 = 7t 2 + 10t + 7 [89]. In this work, the following condensates are included for the QCDSR equations, Now we generalize the above results of SNM to the case of ANM, and the QCDSR equations for the proton are given by [95],…”
Section: Ope Coefficientsmentioning
confidence: 95%
“…The energy dependence of the QCD coupling constant, i.e., α s ≡ g 2 s /4π is given by α s (q 2 ) = 4π/9 ln(q 2 /µ 2 ). The factor L contains radiation effects effectively [95]. Furthermore, the contributions from continuum excitations whose physical origin will be discussed in Section IV, are included by the following functions,…”
Section: Ope Coefficientsmentioning
confidence: 99%
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