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[2]
[Anonymous], describes how to construct bulk invariants in terms of a bulk magnetization operator (in the case of fermionic Fock spaces) but does not obtain explicit formulas for these invariants
[3]
[Anonymous], See Sec. VIII for the definition of Uedge for general MBL Floquet circuits
[4]
[Anonymous], The invariant omegaA,B(U) is closely related to the flow of a unitary matrix
[5]
[Anonymous], We discuss the generalization of our results to fermionic systems