Department of Physics and Astronomy, Johns Hopkins University, Baltimore, Maryland, USA.
Phys Rev Lett. 2009 Oct 30;103(18):187203. doi: 10.1103/PhysRevLett.103.187203. Epub 2009 Oct 28.
Spin excitations in an ordered Heisenberg magnet are magnons-bosons with spin 1. That may change when frustration and quantum fluctuations suppress the order and restore the spin-rotation symmetry. We show that spin excitations in the S=1/2 Heisenberg antiferromagnet on a kagome lattice are spinons-fermions with spin 1/2. In the ground state the system can be described as a collection of small, heavy pairs of spinons with spin 0. A magnetic excitation of lowest energy amounts to breaking up a pair into two spinons at a cost of 0.06 J.
在有序的海森堡磁体中,自旋激发是自旋为 1 的磁振子-玻色子。当受挫和量子涨落抑制有序并恢复自旋-旋转对称性时,这种情况可能会发生变化。我们表明,在 kagome 晶格上的 S=1/2 海森堡反铁磁体中的自旋激发是自旋为 1/2 的自旋子-费米子。在基态下,该系统可以描述为一小部分自旋为 0 的自旋子重对的集合。最低能量的磁激发是将一对自旋子分裂成两个自旋子,代价为 0.06 J。