A first-order Lagrangian theory of fields with arbitrary spin
DOI10.1142/S0219887818500883zbMath1390.81236arXiv1704.01110MaRDI QIDQ4641530
Publication date: 17 May 2018
Published in: International Journal of Geometric Methods in Modern Physics (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/1704.01110
Spinor and twistor methods applied to problems in quantum theory (81R25) Covariant wave equations in quantum theory, relativistic quantum mechanics (81R20) Lagrangian formalism and Hamiltonian formalism in mechanics of particles and systems (70S05) Fiber bundles in algebraic topology (55R10) Quantum mechanics on special spaces: manifolds, fractals, graphs, lattices (81Q35)
Related Items (1)
Cites Work
- Overconnections and the energy-tensors of gauge and gravitational fields
- Natural extensions of electroweak geometry and Higgs interactions
- An algebraic approach to physical scales
- Gauge group of gravity, spinors, and anomalies
- Spinors and diffeomorphisms
- On geometrodynamics with tetrad fields
- On the notions of energy tensors in tetrad-affine gravity
- Two-spinors, field theories and geometric optics in curved spacetime
- Wavefunctions for Particles with Arbitrary Spin
- Positive spaces, generalized semi-densities, and quantum interactions
- Two-spinor geometry and gauge freedom
- TETRAD GRAVITY, ELECTROWEAK GEOMETRY AND CONFORMAL SYMMETRY
- "MINIMAL GEOMETRIC DATA" APPROACH TO DIRAC ALGEBRA, SPINOR GROUPS AND FIELD THEORIES
- Arbitrary spin field equations on curved manifolds with torsion
- Covariant-differential formulation of Lagrangian field theory
- Possibly degenerate tetrad gravity and Maxwell–Dirac fields
- Zur Darstellungstheorie der inhomogenen Lorentzgruppe als Grundlage quantenmechanischer Kinematik
- General relativity with spin and torsion: Foundations and prospects
- Lagrange Anchor for Bargmann–Wigner Equations
- Group Theoretical Discussion of Relativistic Wave Equations
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
This page was built for publication: A first-order Lagrangian theory of fields with arbitrary spin
