Light-front representation of chiral dynamics in peripheral transverse densities

A bstract The nucleon’s electromagnetic form factors are expressed in terms of the transverse densities of charge and magnetization at fixed light-front time. At peripheral transverse distances b  =  O ( M π − 1 ) the densities are governed by chiral dynamics and can be calculated model-independentl...

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Veröffentlicht in:The journal of high energy physics 2015-07, Vol.2015 (7), p.1-42, Article 170
Hauptverfasser: Granados, C., Weiss, C.
Format: Artikel
Sprache:eng
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Zusammenfassung:A bstract The nucleon’s electromagnetic form factors are expressed in terms of the transverse densities of charge and magnetization at fixed light-front time. At peripheral transverse distances b  =  O ( M π − 1 ) the densities are governed by chiral dynamics and can be calculated model-independently using chiral effective field theory (EFT). We represent the leading-order chiral EFT results for the peripheral transverse densities as overlap integrals of chiral light-front wave functions, describing the transition of the initial nucleon to soft pion-nucleon intermediate states and back. The new representation (a) explains the parametric order of the peripheral transverse densities; (b) establishes an inequality between the spin-independent and -dependent densities; (c) exposes the role of pion orbital angular momentum in chiral dynamics; (d) reveals a large left-right asymmetry of the current in a transversely polarized nucleon and suggests a simple interpretation. The light-front representation enables a first-quantized, quantum-mechanical view of chiral dynamics that is fully relativistic and exactly equivalent to the second-quantized, field-theoretical formulation. It relates the charge and magnetization densities measured in low-energy elastic scattering to the generalized parton distributions probed in peripheral high-energy scattering processes. The method can be applied to nucleon form factors of other operators, e.g. the energy-momentum tensor.
ISSN:1029-8479
1126-6708
1029-8479
DOI:10.1007/JHEP07(2015)170