Dimensions and the Generating Functional

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SUMMARY

The dimensions of the generating functional, Z[j], for real scalar field theory are confirmed to be dimensionless. This conclusion arises from the definition of Z[j] as the vacuum-to-vacuum transition amplitude, which equals one when the source j is absent, necessitating a normalization factor in the integration measure, \mathcal{D}\phi. Additionally, the generating functional for connected Green's functions, W[j], is also dimensionless, as it is defined in relation to Z[j] through the equation Z[j]=e^{iW[j]}. This dimensional analysis is applicable beyond field theory, extending to path integrals in non-relativistic quantum mechanics of one particle (NRQMOP).

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  • Understanding of generating functionals in quantum field theory
  • Familiarity with path integrals and their normalization
  • Knowledge of scalar field theory and its mathematical formulations
  • Basic concepts of quantum mechanics, particularly NRQMOP
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The discussion is beneficial for theoretical physicists, quantum field theorists, and students studying quantum mechanics, particularly those interested in the mathematical foundations of generating functionals and their applications in field theory.

TriTertButoxy
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Something seems a little weird to me: What are the dimensions of a generating functional, Z[j] -- say for real scalar field theory?

Z[j]=\int\mathcal{D}\phi\,\exp\, i\!\int d^4x\left(\frac{1}{2}\partial_\mu\phi\partial^\mu\phi-\frac{1}{2}m^2\phi^2+j\phi\right)​

Also, what about mass dimensions of the generating functional for connected Green's functions, W[j]? This is defined in terms of the log of the generating functional, Z[j].

Z[j]=e^{iW[j]}​

This seems a little pathological...
 
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Both Z and W are dimensionless. This is obvious for W, since you couldn't put it into the exponential if it wasn't. As for Z, it's usually defined as the vacuum-to-vacuum transition amplitude in the presence of the source j, and this equals one if there is no source, so Z[0]=1. Thus Z[j] must be dimensionless. To get Z[0]=1, a normalization factor must be implicitly included in the measure over the fields.

None of this is specific to field theory. Similar statements apply to path integrals in NRQMOP (non-relavitistic quantum mechanics of one particle :smile:).
 
Ah, so you mean in order for Z[0]=1, the integration measure, \mathcal{D}\phi, must be normalized such that it is unitless.

I understand now. thanks, Avodyne!
 

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