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23) the monoclinic lattice distortion was not observed in the OPD phase. However, we consider that the (small) local lattice distortions might occur in the OPD phase and therefore the volume fractions of the q domains are conserved in the magnetic phase transition between the PD and OPD phases, because the magnetic structure of the OPD phase breaks the threefold rotational symmetry of the crystal
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23) the monoclinic lattice distortion was not observed in the OPD phase. However, we consider that the (small) local lattice distortions might occur in the OPD phase and therefore the volume fractions of the q domains are conserved in the magnetic phase transition between the PD and OPD phases, because the magnetic structure of the OPD phase breaks the threefold rotational symmetry of the crystal.
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26
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84874172856
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32)). However, we emphasize that a comparison between Figs. 5(a) and 5(b) apparently shows that the multiferroic domain structure (including the asymmetry of the helicity domains in each q domain) after the second cooling cannot be realized by the application of the "uniform" electric field. Therefore, the imperfect conditions mentioned above does not affect the conclusion of the present work
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32)). However, we emphasize that a comparison between Figs. 5(a) and 5(b) apparently shows that the multiferroic domain structure (including the asymmetry of the helicity domains in each q domain) after the second cooling cannot be realized by the application of the "uniform" electric field. Therefore, the imperfect conditions mentioned above does not affect the conclusion of the present work.
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