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Volumn 76, Issue 16, 2007, Pages

Influence of oxygen vacancies on the electronic structure of Hf O2 films

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EID: 35148872144     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.76.165411     Document Type: Article
Times cited : (37)

References (36)
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    • Here the Slater integrals for Hf3+ (d1) / Hf2+ (d2) final states were taken as the reduced values by less than one-half from those calculated for Hf3+ / Hf2+ ion by using Cowan's code for Hartree-Fock method: for Hf3+ (d1), F pd 2 =9.447, G pd 1 =2.187, and G pd 3 =2.239 in eV; and for Hf2+ (d2), F dd 2 =13.102, F pd 4 =9.086, F pd 2 =9.332, G pd 1 =2.124, and G pd 3 =2.183 in eV. Hubbard U and F pd 0 were set to 2 eV and 4 eV, respectively, and the 5d spin-orbit coupling constant was set to about 0.1 eV throughout the calculation. For more details of the calculational method, refer to University of California Press, California
    • Here the Slater integrals for Hf3+ (d1) / Hf2+ (d2) final states were taken as the reduced values by less than one-half from those calculated for Hf3+ / Hf2+ ion by using Cowan's code for Hartree-Fock method: for Hf3+ (d1), F pd 2 =9.447, G pd 1 =2.187, and G pd 3 =2.239 in eV; and for Hf2+ (d2), F dd 2 =13.102, F pd 4 =9.086, F pd 2 =9.332, G pd 1 =2.124, and G pd 3 =2.183 in eV. Hubbard U and F pd 0 were set to 2 eV and 4 eV, respectively, and the 5d spin-orbit coupling constant was set to about 0.1 eV throughout the calculation. For more details of the calculational method, refer to R. D. Cowan, The Theory of Atomic Structure and Spectra (University of California Press, California, 1981).
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    • Cowan, R.D.1


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