The zero-dimensional O(N) vector model as a benchmark for perturbation theory, the large-N expansion and the functional renormalization group
Creators
- 1. Institut für Theoretische Physik, Universität Frankfurt, Max-von-Laue Straße 1, 60438 Frankfurt (Germany)
Description
We consider the zero-dimensional O(N) vector model as a simple example to calculate n-point correlation functions using perturbation theory, the large-N expansion and the functional renormalization group (FRG). Comparing our findings with exact results, we show that perturbation theory breaks down for moderate interactions for all N, as one should expect. While the interaction-induced shift of the free energy and the self-energy are well described by the large-N expansion even for small N, this is not the case for higher order correlation functions. However, using the FRG in its one-particle irreducible formalism, we see that very few running couplings suffice to get accurate results for arbitrary N in the strong coupling regime, outperforming the large-N expansion for small N. We further remark on how the derivative expansion, a well-known approximation strategy for the FRG, reduces to an exact method for the zero-dimensional O(N) vector model. (paper)
Availability note (English)
Available from http://dx.doi.org/10.1088/1751-8113/45/10/105401Additional details
Identifiers
Publishing Information
- Journal Title
- Journal of Physics. A, Mathematical and Theoretical (Online)
- Journal Volume
- 45
- Journal Issue
- 10
- Journal Page Range
- [20 p.]
- ISSN
- 1751-8121
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 43093018
- Subject category
- S97: MATHEMATICAL METHODS AND COMPUTING;
- Descriptors DEI
- APPROXIMATIONS; CORRELATION FUNCTIONS; FREE ENERGY; PERTURBATION THEORY; RENORMALIZATION; SELF-ENERGY; STRONG-COUPLING MODEL; VECTORS
- Descriptors DEC
- CALCULATION METHODS; ENERGY; FUNCTIONS; MATHEMATICAL MODELS; PARTICLE MODELS; PHYSICAL PROPERTIES; TENSORS; THERMODYNAMIC PROPERTIES