scholarly journals Many-body topological invariants for fermionic short-range entangled topological phases protected by antiunitary symmetries

2018 ◽  
Vol 98 (3) ◽  
Author(s):  
Ken Shiozaki ◽  
Hassan Shapourian ◽  
Kiyonori Gomi ◽  
Shinsei Ryu
2020 ◽  
Vol 6 (15) ◽  
pp. eaaz3666 ◽  
Author(s):  
Andreas Elben ◽  
Jinlong Yu ◽  
Guanyu Zhu ◽  
Mohammad Hafezi ◽  
Frank Pollmann ◽  
...  

Many-body topological invariants, as quantized highly nonlocal correlators of the many-body wave function, are at the heart of the theoretical description of many-body topological quantum phases, including symmetry-protected and symmetry-enriched topological phases. Here, we propose and analyze a universal toolbox of measurement protocols to reveal many-body topological invariants of phases with global symmetries, which can be implemented in state-of-the-art experiments with synthetic quantum systems, such as Rydberg atoms, trapped ions, and superconducting circuits. The protocol is based on extracting the many-body topological invariants from statistical correlations of randomized measurements, implemented with local random unitary operations followed by site-resolved projective measurements. We illustrate the technique and its application in the context of the complete classification of bosonic symmetry-protected topological phases in one dimension, considering in particular the extended Su-Schrieffer-Heeger spin model, as realized with Rydberg tweezer arrays.


2016 ◽  
Vol 7 (1) ◽  
Author(s):  
F. Grusdt ◽  
N. Y. Yao ◽  
D. Abanin ◽  
M. Fleischhauer ◽  
E. Demler

2006 ◽  
Vol 97 (23) ◽  
Author(s):  
Hans-Christian Weissker ◽  
Jorge Serrano ◽  
Simo Huotari ◽  
Fabien Bruneval ◽  
Francesco Sottile ◽  
...  

1960 ◽  
Vol 38 (10) ◽  
pp. 1245-1255
Author(s):  
L. E. H. Trainor

A model of the nucleon is described in which a π-meson moves about a nucleon core under the action of a hyper-Maxwell field. On such a model, the short range of the internucleon force appears as a screening effect. Despite its obvious limitations, the model does possess some interesting features which lead to results in agreement with experiment. The advantage to such models is that they may provide insight into problems which are enormously difficult from the usual field theory point of view. In particular, one might hope to obtain some understanding of the state of the π -meson field in the nuclear many-body problem.


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