1981
DOI: 10.1016/0550-3213(81)90303-5
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Are all hadrons alike?

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Cited by 634 publications
(634 citation statements)
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“…We have considered here m s ∼ 200 MeV, but the contribution of this integral is so small that the error due to m s and α s can be neglected. Notice that duality is not supposed to arise in the scalar sector for as low energies as in other channels, due to a probably large contribution from the direct instantons in this sector [35].…”
Section: High-energy Contribution : |S| = Smentioning
confidence: 99%
“…We have considered here m s ∼ 200 MeV, but the contribution of this integral is so small that the error due to m s and α s can be neglected. Notice that duality is not supposed to arise in the scalar sector for as low energies as in other channels, due to a probably large contribution from the direct instantons in this sector [35].…”
Section: High-energy Contribution : |S| = Smentioning
confidence: 99%
“…The parameter α s G 2 represents the central value in the recent determination [17], g 3 G 3 is obtained from the dilute instanton gas model [18], qgGq is extracted from [19], and the dimension-six condensate parameter α s qq 2 is referenced to the vacuum saturation value which is known to underestimate the actual value by up to a factor of 2 in the (I = 1) vector and axial vector channels [20].…”
Section: Fig 1: Feynman Diagrams For the αS-corrections To The Condementioning
confidence: 99%
“…where {a 0 , b 0 , b 1 } are numerical coefficients (see (26)- (28) below), represents the leading condensate contribution to those sum-rules independent of the low-energy theorem [7], and so provide important nonperturbative effects within sum-rule analyses of scalar glueballs. The one-loop coefficients b 0 and b 1 were evaluated in [5] in the absence of quark effects (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…The current J(x) is the lowest-order version of the operator β(α)G 2 (x), which is renormalization-group invariant for chiral quarks [3,4]. As first noted in [5,6], the one-loop gluon condensate contribution to (1)where {a 0 , b 0 , b 1 } are numerical coefficients (see (26)- (28) below), represents the leading condensate contribution to those sum-rules independent of the low-energy theorem [7], and so provide important nonperturbative effects within sum-rule analyses of scalar glueballs. The one-loop coefficients b 0 and b 1 were evaluated in [5] in the absence of quark effects (i.e.…”
mentioning
confidence: 99%