4.7 Article

Contact interaction analysis of pion GTMDs

Journal

EUROPEAN PHYSICAL JOURNAL C
Volume 81, Issue 1, Pages -

Publisher

SPRINGER
DOI: 10.1140/epjc/s10052-020-08791-1

Keywords

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Funding

  1. National Natural Science Foundation of China [11805097, 11175088, 11535005]
  2. Jiangsu Provincial Natural Science Foundation of China [BK20180323]
  3. Jiangsu Province Hundred Talents Plan for Professionals

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The size and shape of GTMDs for pions are largely determined by the scale of emergent hadronic mass, and the hardness of their mass distribution form factor is found to be larger than the electromagnetic form factor, which is in turn harder than the gravitational pressure distribution form factor. The pressure in the vicinity of the pion's core is comparable to that at the center of a neutron star, and the shear pressure reaches its maximum when confinement forces dominate within the pion.
A contact interaction is used to calculate an array of pion twist-two, -three and -four generalised transverse light-front momentum dependent parton distribution functions (GTMDs). Despite the interaction's simplicity, many of the results are physically relevant, amongst them a statement that GTMD size and shape are largely prescribed by the scale of emergent hadronic mass. Moreover, proceeding from GTMDs to generalised parton distributions, it is found that the pion's mass distribution form factor is harder than its electromagnetic form factor, which is harder than the gravitational pressure distribution form factor; the pressure in the neighbourhood of the pion's core is commensurate with that at the centre of a neutron star; the shear pressure is maximal when confinement forces become dominant within the pion; and the spatial distribution of transversely polarised quarks within the pion is asymmetric. Regarding transverse momentum dependent distribution functions, their magnitude and domain of material support decrease with increasing twist. The simplest Wigner distribution associated with the pion's twist-two dressed-quark GTMD is sharply peaked on the kinematic domain associated with valence-quark dominance; has a domain of negative support; and broadens as the transverse position variable increases in magnitude.

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