How to interpret the field function Φ in QFT?

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The field function Φ in Quantum Field Theory (QFT) is interpreted as an operator rather than a wave function due to the nature of second quantization, which eliminates the coordinate representation. This leads to challenges in applying Born's Statistical Interpretation, traditionally associated with wave functions in quantum mechanics. Instead of a wave function, QFT utilizes a wave functional defined on classical configuration space, though it is seldom taught due to its lack of Lorentz covariance. The S-matrix formalism in QFT allows for the calculation of probabilities related to particle scattering, providing insights into particle behavior post-interaction. Overall, while QFT presents complexities in interpretation, it offers robust frameworks for understanding particle dynamics and probabilities.
  • #31
tom.stoer said:
OK, I see. You are right, interpreting this expression in QM it corresponds to a density (like a charge density) in space.

I would never call this density a "density operator" b/c a density operator is already defined in non-rel. QM and its meaning is something totally different

The correct name is (operator-valued) density field.
 
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  • #32
mpv_plate said:
When reading about the basics of QFT I found there is a so called "density operator" which gives the particle density at a given location. It is the combination of annihilation and creation operator in the position space.

Can the density operator be understood as another possible answer? It basically tells where the particles are in the space. When I use the scattering theory it seems I get similar answer: where the particles go (spatially) after they interact (if I understand that correctly). Is the density operator used in the scattering theory?

Yes, the expectation of the density field multiplied by the mass is what becomes in the case of macroscopically many particles the thermodynamical mass density, and tells about where the mass is concentrated.
 

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