2008
DOI: 10.1080/00150190802014438
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Charge Transfer in the Ca1-xSrx HfO3 System

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Cited by 4 publications
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“…Experimentally, both orthorhombic (space group #62, Pnma ) and cubic (space group #221, Pm 3̅ m ) phases of SHO have been reported with lattice parameters a pseudo–cubic = 4.087 Å and a cubic = 4.099 Å, respectively. Since a 2 × 2 × 2 cubic SC (equivalent to a √2 × 1 × √2 SC of orthorhombic SHO) conveniently encompasses an orthorhombically distorted perovskite unit cell, no differences prevail between the defect formation energies of pseudocubic and orthorhombic modification of ABO 3 . , For the SC structures discussed in this work, the lattice parameter of SHO (see Table ) has been optimized with a 12 × 12 × 12 k -mesh, and for the subsequent calculations involving pristine as well as defective SHO, a 40-atom SC (Sr 8 Hf 8 O 24 ) has been derived from the optimized cubic unit cell.…”
Section: Computational Methods and Structural Detailsmentioning
confidence: 99%
“…Experimentally, both orthorhombic (space group #62, Pnma ) and cubic (space group #221, Pm 3̅ m ) phases of SHO have been reported with lattice parameters a pseudo–cubic = 4.087 Å and a cubic = 4.099 Å, respectively. Since a 2 × 2 × 2 cubic SC (equivalent to a √2 × 1 × √2 SC of orthorhombic SHO) conveniently encompasses an orthorhombically distorted perovskite unit cell, no differences prevail between the defect formation energies of pseudocubic and orthorhombic modification of ABO 3 . , For the SC structures discussed in this work, the lattice parameter of SHO (see Table ) has been optimized with a 12 × 12 × 12 k -mesh, and for the subsequent calculations involving pristine as well as defective SHO, a 40-atom SC (Sr 8 Hf 8 O 24 ) has been derived from the optimized cubic unit cell.…”
Section: Computational Methods and Structural Detailsmentioning
confidence: 99%