spin bath
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Quanta ◽  
2021 ◽  
Vol 10 (1) ◽  
pp. 55-64
Author(s):  
Samyadeb Bhattacharya ◽  
Subhashish Banerjee

In this work, we revisit the theory of open quantum systems from the perspective of fermionic baths. Specifically, we concentrate on the dynamics of a central spin half particle interacting with a spin bath. We have calculated the exact reduced dynamics of the central spin and constructed the Kraus operators in relation to that. Further, the exact Lindblad type canonical master equation corresponding to the reduced dynamics is constructed. We have also briefly touched upon the aspect of non-Markovianity from the backdrop of the reduced dynamics of the central spin.Quanta 2021; 10: 55–64.


2021 ◽  
Vol 104 (8) ◽  
Author(s):  
A. A. Wood ◽  
R. M. Goldblatt ◽  
R. P. Anderson ◽  
L. C. L. Hollenberg ◽  
R. E. Scholten ◽  
...  

Author(s):  
Lionel Tenemeza Kenfack ◽  
William Degaulle Waladi Gueagni ◽  
Martin Tchoffo ◽  
Lukong Cornelius Fai

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Tamiro Villazon ◽  
Pieter W. Claeys ◽  
Mohit Pandey ◽  
Anatoli Polkovnikov ◽  
Anushya Chandran

Abstract Long-lived dark states, in which an experimentally accessible qubit is not in thermal equilibrium with a surrounding spin bath, are pervasive in solid-state systems. We explain the ubiquity of dark states in a large class of inhomogeneous central spin models using the proximity to integrable lines with exact dark eigenstates. At numerically accessible sizes, dark states persist as eigenstates at large deviations from integrability, and the qubit retains memory of its initial polarization at long times. Although the eigenstates of the system are chaotic, exhibiting exponential sensitivity to small perturbations, they do not satisfy the eigenstate thermalization hypothesis. Rather, we predict long relaxation times that increase exponentially with system size. We propose that this intermediate chaotic but non-ergodic regime characterizes mesoscopic quantum dot and diamond defect systems, as we see no numerical tendency towards conventional thermalization with a finite relaxation time.


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