Ultraviolet Renormalization and Locality
Ultraviolet renormalization is organized around one structural fact: after subdivergences are treated recursively, short-distance ambiguities are local. They can therefore be absorbed into the finite set of local parameters and field normalizations allowed by the declared symmetries and approximation order. A prediction is complete only after those parameters are fixed by renormalization conditions, the auxiliary regulator is removed or controlled, and the remaining scheme dependence is shown to be beyond the calculated order.
Enter this chapter
Section titled “Enter this chapter”Begin with Ultraviolet Sensitivity and the Renormalization Problem to recognize which short-distance ambiguities require new physical input.
Topics
Section titled “Topics”- Ultraviolet Sensitivity and the Renormalization Problem — Explains why local ultraviolet ambiguities leave a finite number of inputs at fixed order.
- Power Counting of Divergences and Perturbative Renormalizability — Counts possible overall and subgraph divergences.
- QFT Regulator Families and Their Tradeoffs — Compares the symmetry and computational costs of different regulators.
- Dimensional Regularization and Minimal Subtraction — Separates continuation in dimension from the subtraction prescription.
- Local Counterterms and Subdivergence Structure — Explains why remaining ultraviolet ambiguities must be local.
- The R-Operation, Forest Formula, and Overlapping Divergences — Organizes compatible subtractions for nested, disjoint, and overlapping divergences.
- Renormalized Perturbation Theory and Counterterm Rules — Builds finite amplitudes from renormalized parameters and counterterm vertices.
- Symmetry Constraints and the Space of Counterterms — Restricts counterterms using quantum symmetry identities.
- Renormalization Conditions, Schemes, and Finite Parts — Relates finite parameter definitions in different schemes.
- Regulator Removal and Renormalized Predictions — Tests predictions while removing the regulator at fixed renormalized inputs.
How the ideas fit together
Section titled “How the ideas fit together”Power counting identifies candidate counterterms; it does not subtract subdivergences. Forest recursion removes those subdivergences before the remaining local ambiguity is fixed by renormalization conditions. The nonlocal momentum dependence then becomes a prediction. Changing a subtraction scheme changes finite parameter definitions, so comparisons must hold the same physical inputs fixed. Agreement is required through the retained perturbative order, not term by term in bare parameters. This perturbative construction does not itself prove nonperturbative existence. Collins 1984/2023, ch. 5.
Where to go next
Section titled “Where to go next”Continue to Composite Operators and Mixing to understand why local insertions need additional counterterms.
References
Section titled “References”- Collins, John C. 1984; open-access reissue 2023. Renormalization: An Introduction to Renormalization, the Renormalization Group and the Operator-Product Expansion. Cambridge Monographs on Mathematical Physics. Cambridge University Press. DOI and Open PDF.