2007/09/14 by K. Splittorff, J. J. M. Verbaarschot · 3 citations
Mathematics · Physics and Astronomy · #Algorithm #Combinatorics #Computation #Condensed matter physics #Finite volume method #High-Energy Particle Collisions Research #Lattice (music) #Lattice QCD #Limit (mathematics) #Mathematical analysis #Mathematical physics #Mathematics #Order (exchange) #Particle physics #Particle physics theoretical and experimental studies #Phase transition #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Thermodynamic limit #Thermodynamics #hep-lat
paper · pdf · doi:10.1103/physrevd.77.014514
published as Phys.Rev.D77:014514,2008 · 9 pages, 5 figures
arxiv created 2007/09/14 · openalex publication_date 2008/01/29 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
The expectation value of the complex phase factor of the fermion determinant is computed to leading order in the p expansion of the chiral Lagrangian. The computation is valid for \ensuremathμ<m_\ensuremathπ/2 and determines the dependence of the sign problem on the volume and on the geometric shape of the volume. In the thermodynamic limit with Li\ensuremath→\ensuremath∞ at fixed temperature 1/L0, the average phase factor vanishes. In the low temperature limit where Li/L0 is fixed as Li becomes large, the average phase factor approaches 1 for \ensuremathμ<m_\ensuremathπ/2. The results for a finite volume compare well with lattice results obtained by Allton et al. After taking appropriate limits, we reproduce previously derived results for the ϵ regime and for one-dimensional QCD. The distribution of the phase itself is also computed.