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Tensor Network Representation of Many-Body Quantum States and Unitary Operators

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Figure

Figure 2.1: (a) The honeycomb lattice is put on a cylinder with some boundarytensors, Tr
Figure 2.3: Single-line TNR of the toric code state.
Figure 2.4: Double-line TNR of the toric code state. We again split the qubit on eachedge into two, and assign each to the two nearby vertices
Figure 2.5: Numerical calculation of topological entanglement entropy Stopo(ϵ) ofstates represented by toric code fixed point single-line tensors, T0, varied with aninfinitesimal random tensor in different subspaces
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