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In a recent paper (Commun.
1902
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Nonetheless, the timescales necessary to observe the sub-ballistic growth might depend on q q and diverge as q → ∞ q\to\infty
Cited in the paper.
More precisely, it is better to consider the traceless version of the operator, \mathaccentV t i l d e 07 E S j z ≡ 3 ( S j z ) 2 − 2 \mathaccentV{tilde}07E{S}_{j}^{z}\equiv 3\left(S_{j}^{z}\right)^{2}-2
Cited in the paper.
A. Nahum, S. Vijay, and J. Haah, Phys. Rev. X 8
2018
Later among the works it cites.
T. Rakovszky, F. Pollmann, and C. W. von Keyserlingk, Phys. Rev. Lett. 122
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M. Žnidarič, Communications Physics 3
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