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Principles of gauge theory of real hadrons. 3. Lorentz-spinor gauge invariance

Technical Report:

Abstract

Complete classification of relativistically invariant equations of the Gelfand-Yaglom type, which are invariant as regards gauge transformations, generated by bispinor representation of the Lorentz complete group, was devised. 1 ref.
Authors:
Publication Date:
Dec 31, 1992
Product Type:
Technical Report
Report Number:
INP-MSU-92-14-263; NIIYaF-MGU-92-14-263.
Reference Number:
SCA: 662120; 662340; PA: AIX-24:008266; SN: 93000932957
Resource Relation:
Other Information: PBD: 1992
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; HADRONS; LORENTZ INVARIANCE; GAUGE INVARIANCE; IRREDUCIBLE REPRESENTATIONS; ISOSPIN; LAGRANGIAN FUNCTION; MATHEMATICAL SPACE; MATRIX ELEMENTS; MESON-BARYON INTERACTIONS; RELATIVISTIC RANGE; SPINOR FIELDS; 662120; 662340; SYMMETRY, CONSERVATION LAWS, CURRENTS AND THEIR PROPERTIES; HADRON INTERACTIONS
OSTI ID:
10119576
Research Organizations:
Moskovskij Gosudarstvennyj Univ., Moscow (Russian Federation). Nauchno-Issledovatel`skij Inst. Yadernoj Fiziki
Country of Origin:
Russian Federation
Language:
English
Other Identifying Numbers:
Other: ON: DE93613095; TRN: RU9207313008266
Availability:
OSTI; NTIS (US Sales Only); INIS
Submitting Site:
INIS
Size:
[13] p.
Announcement Date:
Jun 30, 2005

Technical Report:

Citation Formats

Slad`, L M. Principles of gauge theory of real hadrons. 3. Lorentz-spinor gauge invariance. Russian Federation: N. p., 1992. Web.
Slad`, L M. Principles of gauge theory of real hadrons. 3. Lorentz-spinor gauge invariance. Russian Federation.
Slad`, L M. 1992. "Principles of gauge theory of real hadrons. 3. Lorentz-spinor gauge invariance." Russian Federation.
@misc{etde_10119576,
title = {Principles of gauge theory of real hadrons. 3. Lorentz-spinor gauge invariance}
author = {Slad`, L M}
abstractNote = {Complete classification of relativistically invariant equations of the Gelfand-Yaglom type, which are invariant as regards gauge transformations, generated by bispinor representation of the Lorentz complete group, was devised. 1 ref.}
place = {Russian Federation}
year = {1992}
month = {Dec}
}