Static electric field in one-dimensional insulators without boundaries

In this brief report, we show that in a one-dimensional insulating system with periodic boundary conditions, the coefficient of the θ term in the effective theory is not only determined by the topological index ∫i∑[superscript α]∈[superscript occ]〈u[superscript k]α|∂/∂k|u[superscript kα]〉dk. Specifi...

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Bibliographic Details
Main Authors: Chen, Kuang-Ting (Contributor), Lee, Patrick A. (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society (APS), 2012-02-17T18:04:37Z.
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Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Chen, Kuang-Ting  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Lee, Patrick A.  |e contributor 
100 1 0 |a Chen, Kuang-Ting  |e contributor 
100 1 0 |a Lee, Patrick A.  |e contributor 
700 1 0 |a Lee, Patrick A.  |e author 
245 0 0 |a Static electric field in one-dimensional insulators without boundaries 
260 |b American Physical Society (APS),   |c 2012-02-17T18:04:37Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/69140 
520 |a In this brief report, we show that in a one-dimensional insulating system with periodic boundary conditions, the coefficient of the θ term in the effective theory is not only determined by the topological index ∫i∑[superscript α]∈[superscript occ]〈u[superscript k]α|∂/∂k|u[superscript kα]〉dk. Specifically, the relative position between the electronic orbitals and the ions also alters the coefficient, as one would expect when one identifies −eθ/2π as the polarization. This resolves a paradox when we apply our previous result to the Su-Shreiffer-Heeger model, where the two ground states related by a lattice translation have θ differed by π. We also show that the static dielectric screening is the same with or without boundaries, in contrast to comments made in our previous paper. 
520 |a National Science Foundation (U.S.) (Grant No. DMR 1104498) 
546 |a en_US 
655 7 |a Article 
773 |t Physical Review B