2013
DOI: 10.1140/epja/i2013-13023-x
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On chiral corrections to nucleon GPD

Abstract: Within the pion-nucleon chiral perturbation theory we derive the leading chiral correction to the nucleon GPD at ξ = 0. We discuss the difficulties of consideration of nonlocal light-cone operators within the theory with a heavy particle and the methods to solve the difficulties. The consideration of the chiral corrections directly for nonlocal operators allows to resolve the ambiguity of the inverse Mellin transformation. In particular, we show that the mixing between axial and vector GPDs are of order m 2 π … Show more

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Cited by 17 publications
(23 citation statements)
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“…(46) and (47), are true to all orders in the pion mass, not just for the LNA parts that were discussed in Refs. [17,18,48], and to which we turn to in the next section.…”
Section: A Pionic Corrections To Twist-2 Matrix Elementsmentioning
confidence: 96%
“…(46) and (47), are true to all orders in the pion mass, not just for the LNA parts that were discussed in Refs. [17,18,48], and to which we turn to in the next section.…”
Section: A Pionic Corrections To Twist-2 Matrix Elementsmentioning
confidence: 96%
“…From the transformation properties of the operators O µ 1 ···µn q and O µ 1 ···µn ∆q under parity [25], the sets of coefficients {α (n) , β (n) , σ (n) , θ (n) , ρ (n) } and {ᾱ (n) ,β (n) ,σ (n) ,θ (n) ,ρ (n) } in (15) are the same as those in the spin-averaged operators in (11).…”
Section: A Operators and Momentsmentioning
confidence: 99%
“…According to the properties of O µ 1 ···µn q and O µ 1 ···µn ∆q under parity transformations [49], the coefficients {α (n) , β (n) , σ (n) } and {ᾱ (n) ,β (n) ,σ (n) } are the same as for the spin-averaged operators in Eq. (25).…”
Section: Matching Coefficients and Pdf Momentsmentioning
confidence: 99%