Local Convertibility and the Quantum Simulation of Edge States in Many-Body Systems

In some many-body systems, certain ground-state entanglement (Rényi) entropies increase even as the correlation length decreases. This entanglement nonmonotonicity is a potential indicator of nonclassicality. In this work, we demonstrate that such a phenomenon, known as lack of local convertibility...

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Main Authors: Franchini, Fabio (Contributor), Cui, Jian (Author), Amico, Luigi (Author), Fan, Heng (Author), Gu, Mile (Author), Korepin, Vladimir (Author), Kwek, Leong Chuan (Author), Vedral, Vlatko (Author)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2014-11-17T17:00:11Z.
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Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Franchini, Fabio  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Franchini, Fabio  |e contributor 
700 1 0 |a Cui, Jian  |e author 
700 1 0 |a Amico, Luigi  |e author 
700 1 0 |a Fan, Heng  |e author 
700 1 0 |a Gu, Mile  |e author 
700 1 0 |a Korepin, Vladimir  |e author 
700 1 0 |a Kwek, Leong Chuan  |e author 
700 1 0 |a Vedral, Vlatko  |e author 
245 0 0 |a Local Convertibility and the Quantum Simulation of Edge States in Many-Body Systems 
260 |b American Physical Society,   |c 2014-11-17T17:00:11Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/91589 
520 |a In some many-body systems, certain ground-state entanglement (Rényi) entropies increase even as the correlation length decreases. This entanglement nonmonotonicity is a potential indicator of nonclassicality. In this work, we demonstrate that such a phenomenon, known as lack of local convertibility, is due to the edge-state (de)construction occurring in the system. To this end, we employ the example of the Ising chain, displaying an order-disorder quantum phase transition. Employing both analytical and numerical methods, we compute entanglement entropies for various system bipartitions (A|B) and consider ground states with and without Majorana edge states. We find that the thermal ground states, enjoying the Hamiltonian symmetries, show lack of local convertibility if either A or B is smaller than, or of the order of, the correlation length. In contrast, the ordered (symmetry-breaking) ground state is always locally convertible. The edge-state behavior explains all these results and could disclose a paradigm to understand local convertibility in other quantum phases of matter. The connection we establish between convertibility and nonlocal, quantum correlations provides a clear criterion of which features a universal quantum simulator should possess to outperform a classical machine. 
520 |a Seventh Framework Programme (European Commission) (Marie Curie International Outgoing Fellowship Grant PIOF-PHY-276093) 
546 |a en 
655 7 |a Article 
773 |t Physical Review X