In the original publication, the captions of Figs. 4 and 5 are correct, but the graphs have been erroneously switched between both figures. In the corrected version below, Fig. 4 correctly shows the result of the lattice-based UC in which the computation times of the ROMs exceed the computation time of the FOM, while Fig. 5 correctly shows the results of the shifted UC in which the computation times of the ROMs are significantly smaller than the computation time of the FOM.

Fig. 4
(a) Dispersion curves of lattice-based UC with underneath relative errors. (b) Computation times of ROM setup and dispersion curve calculation for lattice-based UC. The IBC calculation time is further divided:  denotes the time to apply the Bloch–Floquet BCs (Eq. (3)) and  denotes the time to compute the eigenvalue problem (Eq. (2)).
Fig. 4
(a) Dispersion curves of lattice-based UC with underneath relative errors. (b) Computation times of ROM setup and dispersion curve calculation for lattice-based UC. The IBC calculation time is further divided:  denotes the time to apply the Bloch–Floquet BCs (Eq. (3)) and  denotes the time to compute the eigenvalue problem (Eq. (2)).
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Fig. 5
(a) Dispersion curves of shifted UC with underneath relative errors. (b) Computation times of ROM setup and dispersion curve calculation for shifted UC. A break in the time axis is present. The IBC calculation time is further divided:  denotes the time to apply the Bloch–Floquet BCs (Eq. (3)) and  denotes the time to compute the eigenvalue problem (Eq. (2)).
Fig. 5
(a) Dispersion curves of shifted UC with underneath relative errors. (b) Computation times of ROM setup and dispersion curve calculation for shifted UC. A break in the time axis is present. The IBC calculation time is further divided:  denotes the time to apply the Bloch–Floquet BCs (Eq. (3)) and  denotes the time to compute the eigenvalue problem (Eq. (2)).
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