2015/08/31 by Seyong Kim
Physics and Astronomy · #Bound state #Gauge theory #Lattice (music) #Lattice QCD #Lattice field theory #Lattice gauge theory #Mathematical physics #Particle physics #Particle physics theoretical and experimental studies #Physics #Physics of Superconductivity and Magnetism #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum electrodynamics #Quantum field theory #Quantum mechanics #Wave function #hep-lat #hep-ph
paper · pdf · doi:10.1103/physrevd.92.094505
published as Phys. Rev. D 92, 094505 (2015) · 7 pages, 4 figures
openalex publication_date 2015/11/05 · arxiv created 2015/11/12 · arxiv updated 2015/11/13 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We calculate the bound state properties of stoponium using lattice formulation of nonrelativistic effective field theory for stop which is moving nonrelativistically in the rest frame of stoponium. Our calculation method is similar to that employed in lattice nonrelativistic quantum chromodynamics (NRQCD) studies for charmonium and bottomonium. Using 163\ifmmode×\else\texttimes\fi256 quenched lattice gauge field configurations at a^\ensuremath-1=50(1) GeV, we obtain the stoponium mass and the lattice matrix element which is related to the wave function at the origin for the 1S state and find that the lattice |R1S(0)|2/M1S3 is 3.5--4 larger than that from a potential model calculation for 200 GeV\ensuremath≤M1S\ensuremath≤800 GeV.