2016
DOI: 10.1140/epja/i2016-16114-2
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On the strong coupling N(*)N(*) $\pi$

Abstract: We study the strong vertices N * N π, N * N * π and N N π in QCD, where N * denotes the negative parity N (1535) state. We use the most general form of the interpolating currents to calculate the corresponding strong coupling constants. It is obtained that the coupling associated to N * N π vertex is strongly suppressed compared to those related to two other vertices. The strong coupling corresponding to N * N * π is obtained to be roughly half of that of N N π vertex. We compare the obtained results on N * N … Show more

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Cited by 23 publications
(48 citation statements)
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“…As a result, an opposite mass shift of +45 MeV at ρ 0 was obtained, however, with a significant ambiguity from phenomenological density dependence of the threshold parameter. Recent new analyses [21,22] support the conclusions of [19]. The results of the present paper, obtained by applying the MEM to the QCD sum rules, are independent of uncertainties from phenomenological functional forms and its threshold parameter.…”
Section: Introductionsupporting
confidence: 84%
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“…As a result, an opposite mass shift of +45 MeV at ρ 0 was obtained, however, with a significant ambiguity from phenomenological density dependence of the threshold parameter. Recent new analyses [21,22] support the conclusions of [19]. The results of the present paper, obtained by applying the MEM to the QCD sum rules, are independent of uncertainties from phenomenological functional forms and its threshold parameter.…”
Section: Introductionsupporting
confidence: 84%
“…In this section, we compare our results with those of previous works, which are summarized in Table II. We in particular will comment and shortly discuss the results of the in-medium D meson masses from QCD sum rules [19][20][21][22]. In Ref.…”
Section: Comments For Previous Work In Qcd Sum Rulesmentioning
confidence: 99%
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