2007
DOI: 10.1088/1126-6708/2007/01/039
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Towards a determination of the chiral couplings at NLO in 1/NC: L8r(μ) and C38r(μ)

Abstract: We present a dispersive method which allows to investigate the low-energy couplings of chiral perturbation theory at the next-to-leading order (NLO) in the 1/N C expansion, keeping full control of their renormalization scale dependence. Using the resonance chiral theory Lagrangian, we perform a NLO calculation of the scalar and pseudoscalar twopoint functions, within the single-resonance approximation. Imposing the correct QCD short-distance constraints, one determines their difference Π(t) ≡ Π S (t) − Π P (t)… Show more

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Cited by 58 publications
(142 citation statements)
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References 70 publications
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“…Nonetheless, on the contrary to what happens with other matrix elements (e.g. the S − P correlator [17]), the spin-1 two-point functions do not gain contributions from the U(3)-singlet chiral pseudo-Goldstone; the η 1 does neither enter at tree-level nor in the one-loop correlators. Therefore, the corresponding LECs are identical in both theories at leading and next-to-leading order in 1/N C :…”
Section: Phenomenologymentioning
confidence: 80%
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“…Nonetheless, on the contrary to what happens with other matrix elements (e.g. the S − P correlator [17]), the spin-1 two-point functions do not gain contributions from the U(3)-singlet chiral pseudo-Goldstone; the η 1 does neither enter at tree-level nor in the one-loop correlators. Therefore, the corresponding LECs are identical in both theories at leading and next-to-leading order in 1/N C :…”
Section: Phenomenologymentioning
confidence: 80%
“…[17,18], our results can be also derived in an utterly equivalent way through a Feynman diagram computation and the standard renormalization procedure. This derivation is slightly more complex and its detailed explaination is relegated to appendix E.…”
Section: The Vector Form Factor Of the Pionmentioning
confidence: 85%
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