captain
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are bosons represented by a scalar field and fermions represented by a spin 1/2 field or how does it work?
The discussion revolves around the representation of bosons and fermions in quantum field theory, specifically focusing on scalar fields, spin-1/2 fields, and the properties of different spin fields. The scope includes theoretical concepts and technical explanations related to particle physics.
Participants generally agree on the classification of bosons and fermions and the nature of scalar and spin-1/2 fields. However, there are nuances regarding the representation of spin-3/2 particles and the specifics of propagators that remain less settled.
Some discussions touch on the complexities of spin-3/2 theories and their limitations in perturbation theory, indicating unresolved mathematical and theoretical challenges.
Bosons have integer spin (0,1,2...). Fermions have half-integer spin (1/2, 3/2, ...)captain said:are bosons represented by a scalar field and fermions represented by a spin 1/2 field or how does it work?
strangerep said:Bosons have integer spin (0,1,2...). Fermions have half-integer spin (1/2, 3/2, ...)
A scalar field is a spin zero field. For spin one you'd need a vector field and for spin two you'd need a second rank tensor field.captain said:does that mean a scalar field is a spin zero field or is it an integer spin field?
Son Goku said:A scalar field is a spin zero field. For spin one you'd need a vector field and for spin two you'd need a second rank tensor field.
A spin-1/2 particle is described using a Lorentz/Dirac Spinor Field. There are no “fundamental” spin-3/2 particles so the field that would describe it isn’t used that often. However if you know representation theory you can easily see what the field’s properties are like.captain said:what about a spin 1/2 or spin 3/2?
Yes, there is a different propagator for each field as they have different Hamiltonians. There is also a different Feynman propagator for each free particle species of a given spin.*captain said:is there a different propagator for each spin field?