2014/09/30 by Johannes Richter, J. Richter, Ronald Zinke +2 · 1 citation
Physics and Astronomy · #Advanced Condensed Matter Physics #Band gap #Condensed matter physics #Electron #Ferromagnetism #Gapless playback #Ground state #Heisenberg model #Ising model #Lattice (music) #Paramagnetism #Physics #Physics of Superconductivity and Magnetism #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #Quantum spin liquid #Spin (aerodynamics) #Spin model #Spin polarization #Square lattice #cond-mat.str-el
paper · pdf · doi:10.1140/epjb/e2014-50589-x
published as Eur. Phys. J. B 88, 2 (2015) · 10 pages, 3 figures, accepted version
arxiv created 2014/11/25 · openalex publication_date 2015/01/01 · arxiv updated 2015/01/16 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We use the coupled cluster method to high orders of approximation in order to calculate the ground-state energy, the ground-state magnetic order parameter, and the spin gap of the spin-1/2 J1-J2 model on the square lattice. We obtain values for the transition points to the magnetically disordered quantum paramagnetic phase of J2c1=0.454J1 and J2c2= 0.588 J1. The spin gap is zero in the entire parameter region accessible by our approach, i.e. for J2 ≤ 0.49J1 and J2 > 0.58J1. This finding is in favor of a gapless spin-liquid ground state in this parameter regime.