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Computing hadronic matrix elements of currents is particularly simple
on the light-front, since they can be obtained rigorously as overlaps
of light-front wave functions as in the
formula.<ref name="Drell:1969km">{{ cite journal |author1=S. D. Drell |author2=T. -M. Yan |
title= Connection of Elastic Electromagnetic Nucleon Form-Factors at Large <math>Q^2</math> and Deep Inelastic Structure Functions Near Threshold |
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of light-front time-ordered [[Perturbation theory (quantum mechanics)|perturbation theory]],
together with <math>J^z</math> conservation, can be used
to elegantly derive the
amplitudes.<ref name="Cruz-Santiago:2013vta">{{ cite journal |author1=C. A. Cruz-Santiago |author2=A. M. Stasto |
title= Recursion relations and scattering amplitudes in the light-front formalism |
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doi= 10.1016/0550-3213(95)00009-H|arxiv = hep-ph/9401328 |bibcode = 1995NuPhB.441..197B |s2cid=118969788 }}</ref>
behavior of structure functions
at large <math>x</math> and
duality<ref name="BloomGilman1">{{ cite journal |author1=E. Bloom |author2=F. Gilman |
title= Scaling, Duality, and the Behavior of Resonances in Inelastic electron-Proton Scattering |
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interactions. It is called a helicity because the spin quantization
axis is determined by the orientation of the light front. It differs
from the
determined by the direction of the momentum.
Line 1,211:
lines.
* Construct symmetry-preserving regularization and renormalization schemes for light-front QCD, to include the
title=Comparison of quantum field perturbation theory for the light front with the theory in lorentz coordinates |
journal=[[Theoretical and Mathematical Physics]] | volume= 112 |issue=3 | pages= 1117–1130 | year=1997 |
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matrix elements that involve boosts, such as the
ones needed to calculate form factors. The
relation to covariant
projected on the light-front may help in
understanding the angular momentum issue and its
|