2007/04/30 by Diego Guerra, Diana Belkis Gómez Guerra, R. Méndez–Galain +3 · 3 citations
Mathematics · Physics and Astronomy · #Critical exponent #Criticality #Exponent #Geometry #High-Energy Particle Collisions Research #Mathematical physics #Mathematics #Momentum (technical analysis) #Non-perturbative #Order (exchange) #Particle physics theoretical and experimental studies #Phase transition #Physics #Quantum #Quantum Chromodynamics and Particle Interactions #Quantum gravity #Quantum mechanics #Renormalization #Renormalization group #Scalar (mathematics) #Scalar field theory #Statistical physics #cond-mat.stat-mech #hep-th
paper · pdf · doi:10.1140/epjb/e2007-00296-x
published as Eur.Phys.J.B59:357-365,2007 · 20 pages, 6 figures. Minor changes. Version to be published in EPJ B
openalex publication_date 2007/10/01 · arxiv created 2007/10/23 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The usual procedure of including a finite number of vertices in Non Perturbative Renormalization Group equations in order to obtain n-point correlation functions at finite momenta is analyzed. This is done by exploiting a general method recently introduced which includes simultaneously all vertices although approximating their momentum dependence. The study is performed using the self-energy of the tridimensional scalar model at criticality. At least in this example, low order truncations miss quantities as the critical exponent η by as much as 60%. However, if one goes to high order truncations the procedure seems to converge rapidly.