Henley Christopher L
Laboratory of Atomic and Solid State Physics, Cornell University, Ithaca, New York 14853-2501, USA.
Phys Rev Lett. 2006 Feb 3;96(4):047201. doi: 10.1103/PhysRevLett.96.047201. Epub 2006 Jan 30.
The (three-dimensional) pyrochlore lattice antiferromagnet with Heisenberg spins of large spin length S is a highly frustrated model with a macroscopic degeneracy of classical ground states. The zero-point energy of (harmonic-order) spin-wave fluctuations distinguishes a subset of these states. I derive an approximate but illuminating effective Hamiltonian, acting within the subspace of Ising spin configurations representing the collinear ground states. It consists of products of Ising spins around loops, i.e., has the form of a Z2 lattice gauge theory. The remaining ground-state entropy is still infinite but not extensive, being O(L) for system size O(L3). All these ground states have unit cells bigger than those considered previously.
具有大自旋长度(S)的海森堡自旋的(三维)烧绿石晶格反铁磁体是一个高度受挫的模型,其经典基态具有宏观简并性。(谐波阶)自旋波涨落的零点能量区分了这些态的一个子集。我推导了一个近似但具有启发性的有效哈密顿量,它作用于表示共线基态的伊辛自旋构型子空间内。它由围绕回路的伊辛自旋乘积组成,即具有(Z_2)晶格规范理论的形式。剩余的基态熵仍然是无穷大但非广延的,对于系统大小为(O(L^3))时为(O(L))。所有这些基态的晶胞都比之前考虑的更大。