English

Discrete Higher Berry Phases and Matrix Product States

Strongly Correlated Electrons 2023-04-18 v2 Superconductivity High Energy Physics - Theory Mathematical Physics math.MP Quantum Physics

Abstract

A 11-parameter family of invertible states gives a topological transport phenomenon, similar to the Thouless pumping. As a natural generalization of this, we can consider a family of invertible states parametrized by some topological space XX. This is called a higher pump. It is conjectured that (1+1)(1+1)-dimensional bosonic invertible state parametrized by XX is classified by H3(X;Z)\mathrm{H}^{3}(X;\mathbb{Z}). In this paper, we construct two higher pumping models parametrized by X=RP2×S1X=\mathbb{R}P^{2}\times S^1 and X=L(3,1)×S1X=\mathrm{L}(3,1)\times S^1 that corresponds to the torsion part of H3(X;Z)\mathrm{H}^{3}(X;\mathbb{Z}). As a consequence of the nontriviality as a family, we find that a quantum mechanical system with a nontrivial discrete Berry phase is pumped to the boundary of the (1+1)(1+1)-dimensional system. We also study higher pump phenomena by using matrix product states (MPS), and construct a higher pump invariant which takes value in a torsion part of H3(X;Z)\mathrm{H}^{3}(X;\mathbb{Z}). This is a higher analog of the ordinary discrete Berry phase that takes value in the torsion part of H2(X;Z)\mathrm{H}^{2}(X;\mathbb{Z}). In order to define the higher pump invariant, we utilize the smooth Deligne cohomology and its integration theory. We confirm that the higher pump invariant of the model has a nontrivial value.

Keywords

Cite

@article{arxiv.2303.04252,
  title  = {Discrete Higher Berry Phases and Matrix Product States},
  author = {Shuhei Ohyama and Yuji Terashima and Ken Shiozaki},
  journal= {arXiv preprint arXiv:2303.04252},
  year   = {2023}
}

Comments

40 pages, 21 figures