Subsidiary conditions of the general Gel'fand-Yaglom wave equation based on the representation (1/2,3/2)\(\oplus (-1/2,3/2)\oplus (1/2,5/2)\oplus (-1/2,5/2)\oplus (1/2,3/2)\oplus (-1/2,3/2)\)

DOI10.1007/BF00671685zbMath0634.35061MaRDI QIDQ1096794

C. G. Koutroulos

Publication date: 1986

Published in: International Journal of Theoretical Physics (Search for Journal in Brave)

zbMATH Keywords

representationexternal electromagnetic fieldGel'fand-Yaglom wave equationspinor formsubsidiary conditions

Mathematics Subject Classification ID

Partial differential equations of mathematical physics and other areas of application (35Q99)

Related Items (1)

General necessary conditions for the derivation of the secondary constraints of a first-order relativistic wave equation

Cites Work

• Inconsistency of the local field theory of charged spin 3/2 particles
• Invariant wave equations. Proceedings of the Ettore Majorana international school of mathematical physics held in Erice, June 27 to July 9, 1977
• Propagation of Nonlinear Electromagnetic Field Theories
• On a Theory of Particles with Half-Integral Spin
• Fierz-Pauli Theory of Particles of Spin<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mfrac><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mfrac></mml:math>

This page was built for publication: Subsidiary conditions of the general Gel'fand-Yaglom wave equation based on the representation (1/2,3/2)\(\oplus (-1/2,3/2)\oplus (1/2,5/2)\oplus (-1/2,5/2)\oplus (1/2,3/2)\oplus (-1/2,3/2)\)