Wave-function renormalization rescales a field so that its kinetic term or propagator residue has the chosen normalization. Its scale dependence gives the field's anomalous dimension.
Canonical field normalization rescales a field so that its kinetic term has unit coefficient. For a chiral superfield with K=ZΦ†Φ, the change Φc=Z1/2Φ turns holomorphic superpotential parameters into canonical parameters mc=m/Z and gc=g/Z3/2.
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- Renormalization
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- Anomalous dimension
- Asymptotic scalar field
- Holomorphic and canonically normalized superpotential couplings
- Holomorphic gauge coupling
- Momentum-cutoff two-point function in six-dimensional cubic scalar theory
- Non-renormalization theorem
- One-loop massive phi-fourth counterterms
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- Perturbative gauge-coupling independence of the Wilsonian superpotential
- Perturbative renormalizability of cubic scalar theory in six dimensions
- Sunset diagram
- Ward identity for QED renormalization constants
- Wick-rotated cutoff tadpole mass shift
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