Pairs in the light-front and covariance
read the original abstract
The electromagnetic current of bound systems in the light-front is constructed in the Breit-Frame, in the limit of momentum transfer $q^+=(q^0+q^3)$ vanishing. In this limit, the pair creation term survives and it is responsible for the covariance of the current. The pair creation term is computed for the $j^+$ current of a spin one composite particle in the Breit-frame. The rotational symmetry of $j^+$ is violated if the pair term is not considered.
This paper has not been read by Pith yet.
Forward citations
Cited by 3 Pith papers
-
Chirality Transfer to the Magnetic Sublattice in the Hybrid Perovskite (R)-/(S)-3-Fluoropyrrolidinium Copper(II) Chloride
Chiral organic cations induce chiral magnetic order in a centrosymmetric Cu-Cl inorganic sublattice, shown by a second-order magnetoelectric effect present only in the enantiopure (R/S) variants and absent in the race...
-
Chirality Transfer to the Magnetic Sublattice in the Hybrid Perovskite (R)-/(S)-3-Fluoropyrrolidinium Copper(II) Chloride
Chiral organic cations induce chiral magnetic order and a second-order magnetoelectric effect in a 2D copper(II) chloride hybrid perovskite, while the racemic variant shows neither.
-
Light-front mass operator with dressed quarks
An effective dressed light-front mass operator for quarks is constructed from a lattice-inspired propagator and applied to compute pion TMDs, PDFs, and distribution amplitudes.
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.