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Geometric  relaxations  are done by keeping the in-plane lattice parameter ¡®a¡¯ fixed and relaxing the out-of-plane lattice parameter
¡®c¡¯. An  external  stress  has  been  applied  along  the  c  axis  in  order  to
compensate for the overestimation of cell volume.
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»¹ÓÐÁíһƪÎÄÕÂÖУºBefore we proceed we note that calculations with GGA+U overestimate lattice constant a by ~1%¡£Therefore £¬ we introduce a shift
of the zero for sigma33, the out-of-plane component of the stress, so that sigma33 =0 for the cubic structure at the experimental lattice constant.
Thus, the correct cubic structure is obtained at misfit strain =[a£¨exp£©-a]/a£¨exp£©=0 .
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µÚһƪÎÄÕÂReversible control of magnetic interactions by electric field in a single-phase material
              Nature Communications 4, Article number: 1334 doi:10.1038/ncomms2329
               Published 08 January 2013
µÚ¶þƪÎÄÕÂMagnetic and Electric Phase Control in Epitaxial EuTiO3 from First Principles
                Phys. Rev. Lett. 97, 267602 ¨C Published 29 December 2006

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