本文利用 Onsager 代数为可积 N 态 chiral-clock 模型引入枢轴过程,揭示 D_{2N} 对称性导致的偶数 N SPT 与奇数 N RSPT 序,并分析其基态、纠缠谱及丰富相图。
摘要:
Onsager 代数最初为求解二维 Ising 模型而提出,可用于为一族可积的 N 态 chiral-clock 模型构造守恒荷。我们展示它如何自然地为这一族手征 Hamilton 量产生一种“枢轴”过程。这些 Hamilton 量具有反幺正 CPT 对称性,当它与通常的 Z_N clock 对称性结合时,会给出非阿贝尔二面体对称群 D_{2N}。我们证明,该对称性使这一家族在所有偶数 N 下产生对称性保护拓扑(SPT)序,并在所有奇数 N 下产生表示-SPT(RSPT)物理。最简单的例子是一条次近邻链,它推广了 spin-1/2 cluster 模型,属于一种 SPT 物相。我们推导了其不动点基态的矩阵乘积态表示,以及随之而来的纠缠谱和对称分数化。我们分析了将该模型与 Onsager 可积 chiral Potts 链结合所得的丰富相图,发现了平庸、对称性破缺和(R)SPT 序,以及扩展的无隙区域。对于奇数 N,从 SPT 的观点看,这些相变“不必要地”具有临界性。
英文摘要:
The Onsager algebra, invented to solve the two-dimensional Ising model, can be used to construct conserved charges for a family of integrable $N$-state chiral clock models. We show how it naturally gives rise to a "pivot" procedure for this family of chiral Hamiltonians. These Hamiltonians have an anti-unitary CPT symmetry that when combined with the usual $\mathbb{Z}_N$ clock symmetry gives a non-abelian dihedral symmetry group $D_{2N}$. We show that this symmetry gives rise to symmetry-protected topological (SPT) order in this family for all even $N$, and representation-SPT (RSPT) physics for all odd $N$. The simplest such example is a next-nearest-neighbour chain generalising the spin-1/2 cluster model, an SPT phase of matter. We derive a matrix-product state representation of its fixed-point ground state along with the ensuing entanglement spectrum and symmetry fractionalisation. We analyse a rich phase diagram combining this model with the Onsager-integrable chiral Potts chain, and find trivial, symmetry-breaking and (R)SPT orders, as well as extended gapless regions. For odd $N$, the phase transitions are "unnecessarily" critical from the SPT point of view.
Charge pumps, pivot Hamiltonians and symmetry-protected topological phases
St John’s College and Mathematical Institute, University of Oxford(牛津大学圣约翰学院和数学研究所);Mani L. Bhaumik Institute for Theoretical Physics, Department of Physics and Astronomy, University of California, Los Angeles(加州大学洛杉矶分校物理与天文学系曼尼·L·鲍姆克理论物理研究所);Pritzker School of Molecular Engineering, University of Chicago(芝加哥大学普利策分子工程学院);Harish-Chandra Research Institute(哈里什-昌德拉研究所)