Shannon Nic, Momoi Tsutomu, Sindzingre Philippe
Max-Planck-Institut für Chemische Physik fester Stoffe, Nöthnitzer Strasse 40, 01187 Dresden, Germany.
Phys Rev Lett. 2006 Jan 20;96(2):027213. doi: 10.1103/PhysRevLett.96.027213. Epub 2006 Jan 19.
We present a new scenario for the breakdown of ferromagnetic order in a two-dimensional quantum magnet with competing ferromagnetic and antiferromagnetic interactions. In this, dynamical effects lead to the formation of two-magnon bound states, which undergo Bose-Einstein condensation, giving rise to bond-centered nematic order. This scenario is explored in some detail for an extended Heisenberg model on a square lattice. In particular, we present numerical evidence confirming the existence of a state with d-wave nematic correlations but no long-range magnetic order, lying between the saturated ferromagnetic and collinear antiferromagnetic phases of the ferromagnetic model J1-J2. We argue by continuity of spectra that this phase is also present in a model with 4-spin cyclic exchange.
我们提出了一种新的情景,用于解释具有铁磁和反铁磁相互作用竞争的二维量子磁体中铁磁序的破坏。在这种情景中,动力学效应导致两磁振子束缚态的形成,这些束缚态经历玻色-爱因斯坦凝聚,从而产生以键为中心的向列序。我们针对正方晶格上的扩展海森堡模型对这一情景进行了详细探讨。特别地,我们给出了数值证据,证实了在铁磁模型J1-J2的饱和铁磁相和共线反铁磁相之间存在一种具有d波向列关联但无长程磁序的状态。我们通过谱的连续性论证,在具有4自旋循环交换的模型中也存在这一相。