Fig. 6: Tensor network diagram depicting a maximally entangling orbital rotation circuit.
A sequence of \(\frac{\pi }{2}\) and \(\frac{\pi }{4}\) orbital rotations transforms the unentangled state \({\left\vert 1\right\rangle }^{\otimes {N}_{A}}\otimes {\left\vert 0\right\rangle }^{\otimes {N}_{B}}\) to a state with maximal Schmidt rank and von Neumann entropy across the A/B partition, where NA = NB = N/2, shown above for N = 6 and explained in Supplementary Note 4.
