In 1938, Stueckelberg introduced a scalar field which makes an Abelian gauge theory
massive but preserves gauge invariance. The Stueckelberg mechanism is the introduction of …

We review the present state of knowledge regarding the transverse polarisation (or
transversity) distributions of quarks. After some generalities on transverse polarisation, we …

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Help 50+ years of INIS International Nuclear Information System International Nuclear …

We present the next-to-next-to-leading order (NNLO) corrections to the total cross section for
(pseudo-) scalar Higgs boson production using an alternative method than those used in …

A bstract Future high luminosity polarized deep-inelastic scattering experiments will improve
both the knowledge of the spin sub-structure of the nucleons and contribute further to the …

These lectures describe in detail the effective Hamiltonians for weak decays of mesons
constructed by means of the operator product expansion and the renormalization group …

We calculate next-to-leading QCD corrections to the effective hamiltonian for weak decays in
the limit of massless quarks using three regularization schemes with different treatment of γ …

In this paper we present a calculation of the ΔS= 1 effective weak hamiltonian including next-
to-leading order QCD and QED corrections. At a scale μ of the order of a few GeV, the …

We show that a fully anticommuting γ 5 is a correct and natural prescription for the
dimensional regularization of one fermion loop graphs in spontaneously broken gauge …

Polarized and unpolarized prompt photon production beyond the leading order Page 1
PHYSICAL REVIEW D VOLUME 48, NUMBER 7 1 OCTOBER 1993 Polarized and unpolarized …