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Fixing the quantum three-point function

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Figure

Figure 1: Corner transfer matrix (CTM) acting on a spin chain. We assume an infinite lattice on the right hand side
Figure 2: Structure of contractions captured by the operator O 12 defined by (5.9) and by the vector h↑ L
Figure 3: The Riemann surface for the three quasimomenta in the u- u-parametrization. For simplicity we assumed one-cut solutions

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