On the Manifestation for Longitudinally Polarized
arXiv:hep-ph/9405228 · doi:10.1103/PhysRevD.51.25
Abstract
The contribution of the structure function to polarized deep inelastic scattering is slightly redefined in order to avoid kinematical zeros. Its strong -dependence implied by the Burkhardt-Cottingham (BC) sum rule naturally explains the sign change of the generalized Gerasimov-Drell-Hearn (GDH) sum rule. The status of the BC sum rule and implications for other spin processes are discussed.
16 pages,CPT-94/P.3014,latex
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Cited by in corpus (18)
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- Leading and higher twists in the proton polarized structure function at large Bjorken x
- Measurement of Inclusive Spin Structure Functions of the Deuteron
- Bjorken polarized sum rule and infrared-safe QCD couplings
- QCD radiative and power corrections and Generalized GDH sum rules
- The Q^2-dependence of the Generalised Gerasimov-Drell-Hearn Integral for the Proton
- The Generalized Gerasimov-Drell-Hearn Integral and the Spin Structure of the Nucleon
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- Comment on the Burkhardt - Cottingham and Generalized Gerasimov-Drell-Hearn Sum Rules for the neutron
- Gluon polarization in transversely polarized nucleons and jet spin asymmetries at RHIC
- Spin Response of the Nucleon in the Resonance Region
- The elastic contribution to the Burkhardt -- Cottingham and Generalized Gerasimov--Drell-Hearn Sum Rules