A universal flow invariant in quantum field theory
arXiv:hep-th/0101088 · doi:10.1088/0264-9381/18/21/304
Abstract
A flow invariant is a quantity depending only on the UV and IR conformal fixed points and not on the flow connecting them. Typically, its value is related to the central charges a and c. In classically-conformal field theories, scale invariance is broken by quantum effects and the flow invariant a_{UV}-a_{IR} is measured by the area of the graph of the beta function between the fixed points. There exists a theoretical explanation of this fact. On the other hand, when scale invariance is broken at the classical level, it is empirically known that the flow invariant equals c_{UV}-c_{IR} in massive free-field theories, but a theoretical argument explaining why it is so is still missing. A number of related open questions are answered here. A general formula of the flow invariant is found, which holds also when the stress tensor has improvement terms. The conditions under which the flow invariant equals c_{UV}-c_{IR} are identified. Several non-unitary theories are used as a laboratory, but the conclusions are general and an application to the Standard Model is addressed. The analysis of the results suggests some new minimum principles, which might point towards a better understanding of quantum field theory.
28 pages, 3 figures; proof-corrected version for CQG
References in corpus (6)
- The Supergravity Dual of N=1 Super Yang-Mills Theory
- Anomalies, Unitarity and Quantum Irreversibility
- A Note on the Holographic Beta and C Functions
- Quantum irreversibility in arbitrary dimension
- Towards the classification of conformal field theories in arbitrary even dimension
- Irreversibility and higher-spin conformal field theory
Cited by in corpus (4)
- Inequalities for trace anomalies, length of the RG flow, distance between the fixed points and irreversibility
- Holographic RG flows, entanglement entropy and the sum rule
- Search for flow invariants in even and odd dimensions
- A note on the improvement ambiguity of the stress tensor and the critical limits of correlation functions