Pole term and gauge invariance in deep inelastic scattering
Description
In this paper the authors reconcile two contradictory statements about deep inelastic scattering (DIS) in manifestly covariant theories: (1) the scattering must be gauge invariant, even in the deep inelastic limit, and (2) the pole term (which is not gauge invariant in a covariant theory) dominates the scattering amplitude in the deep inelastic limit. An ''intermediate'' answer is found to be true. They show that, at all energies, the gauge dependent part of the pole term cancels the gauge dependent part of the rescattering term, so that both the pole and rescattering terms can be separately redefined in a gauge invariant fashion. The resulting, redefined pole term is then shown to dominate the scattering in the deep inelastic limit. Details are worked out for a simple example in 1+1 dimensions
Availability note (English)
Available from PURL: https://www.osti.gov/servlets/purl/755922-2kgq82/webviewable/Additional details
Identifiers
Publishing Information
- Imprint Pagination
- 803 Kilobytes
- Report number
- DOE/ER--40150-1497
INIS
- Country of Publication
- United States
- Country of Input or Organization
- United States
- INIS RN
- 31030445
- Subject category
- S72: PHYSICS OF ELEMENTARY PARTICLES AND FIELDS;
- Resource subtype / Literary indicator
- Non-conventional Literature
- Descriptors DEI
- DEEP INELASTIC SCATTERING; DIMENSIONS; GAUGE INVARIANCE; HADRONS; LEPTON-HADRON INTERACTIONS; PARTICLE STRUCTURE; QUARK MODEL; SCATTERING AMPLITUDES; STRUCTURE FUNCTIONS
- Descriptors DEC
- AMPLITUDES; COMPOSITE MODELS; ELEMENTARY PARTICLES; FUNCTIONS; INELASTIC SCATTERING; INTERACTIONS; INVARIANCE PRINCIPLES; LEPTON-BARYON INTERACTIONS; LEPTON-HADRON INTERACTIONS; LEPTON-NUCLEON INTERACTIONS; MATHEMATICAL MODELS; PARTICLE INTERACTIONS; PARTICLE MODELS; SCATTERING
Optional Information
- Contract/Grant/Project number
- AC--05-84ER40150
- Notes
- Submitted to Phys.Rev. C58 (1998) 2963-2976
- Funding organization
- USDOE Office of Energy Research (ER) (United States)
- Secondary number(s)
- JLAB-THY--98-13; WM--98-101; Nucl-th--9803053