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mic(r)-ε is the difference between the microscopic and macroscopic fields.
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43
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17044379154
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note
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The accuracy of the lattice susceptibility when computed in this manner depends on the fit of the energy expansion coefficients in Eq. (6). At compressive strains near the ferroelectric phase transition, the energy as expressed in Eq. (4) has a very small quadratic coefficient b, and is thus increasingly difficult to fit reliably. This is especially problematic because, as can be seen from Eqs. (6) and (11), the dielectric constant in zero electric field depends only on the quadratic term in the energy expansion. Thus, for compressive strains larger than 0.4%, we adjust b so that the zero-field dielectric constant obtained from (11) agrees with that obtained from DFPT. For these strain values, only the fourth order coefficient d is fitted using the energy expansion.
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