lattice fermion
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2021 ◽  
Vol 104 (9) ◽  
Author(s):  
Xingyu Guo ◽  
Chen-Te Ma ◽  
Hui Zhang
Keyword(s):  

Axioms ◽  
2020 ◽  
Vol 9 (3) ◽  
pp. 90
Author(s):  
Kazuki Yamaga

It is known that, in quantum theory, measurements may suppress Hamiltonian dynamics of a system. A famous example is the ‘Quantum Zeno Effect’. This is the phenomena that, if one performs the measurements M times asking whether the system is in the same state as the one at the initial time until the fixed measurement time t, then survival probability tends to 1 by taking the limit M→∞. This is the case for fixed measurement time t. It is known that, if one takes measurement time infinite at appropriate scaling, the ‘Quantum Zeno Effect’ does not occur and the effect of Hamiltonian dynamics emerges. In the present paper, we consider the long time repeated measurements and the dynamics of quantum many body systems in the scaling where the effect of measurements and dynamics are balanced. We show that the stochastic process, called the symmetric simple exclusion process (SSEP), is obtained from the repeated and long time measurements of configuration of particles in finite lattice fermion systems. The emerging stochastic process is independent of potential and interaction of the underlying Hamiltonian of the system.


2018 ◽  
Vol 121 (19) ◽  
Author(s):  
Xiao-Qi Sun ◽  
Meng Xiao ◽  
Tomáš Bzdušek ◽  
Shou-Cheng Zhang ◽  
Shanhui Fan

2018 ◽  
Vol 2 (2) ◽  
pp. 025031
Author(s):  
J Skolimowski ◽  
D Vollhardt ◽  
K Byczuk

2018 ◽  
Vol 59 (2) ◽  
pp. 022301 ◽  
Author(s):  
Michael O’Carroll ◽  
Paulo A. Faria da Veiga

2018 ◽  
Vol 175 ◽  
pp. 03004 ◽  
Author(s):  
David Schaich ◽  
Simon Catterall

We present ongoing investigations of a four-dimensional lattice field theory with four massless reduced staggered fermions coupled through an SU(4)-invariant fourfermion interaction. As in previous studies of four-fermion and Higgs–Yukawa models with different lattice fermion discretizations, we observe a strong-coupling phase in which the system develops a mass gap without breaking any lattice symmetry. This symmetric strong-coupling phase is separated from the symmetric weak-coupling phase by a narrow region of four-fermi coupling in which the system exhibits long-range correlations.


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