“…In this case we find a higher defect formation energy for the F þ center than for the F center for the unrelaxed system. This result is in qualitative agreement with the calculated data of Scorza et al [36] who used the EMBED program [38,39] at the HF level in combination with second order Møller-Plesset theory for an estimate of the correlation energy.…”
Section: The Neutral and Charged Oxygen Vacancysupporting
Single neutral and positively charged oxygen vacancies (F and F þ centers) in a-Al 2 O 3 are investigated using the supercell model (SCM) at the Hartree-Fock (HF) and density functional theory (DFT) level and the cyclic cluster model (CCM) implemented in the semiempirical MSINDO method. Results of supercell and cyclic cluster calculations for the cohesive energy of the perfect Al 2 O 3 crystal are compared with the experimental value for the heat of atomization. The defect formation energy of the unrelaxed F center is calculated with the SCM. The CCM is used to calculate the defect formation energy of the F and the F þ centers. Relaxation effects for the nearest neighbors (NN) and the nextnearest neighbors (NNN) of the F and F þ centers are investigated. The obtained values are compared to other theoretical literature data.
“…In this case we find a higher defect formation energy for the F þ center than for the F center for the unrelaxed system. This result is in qualitative agreement with the calculated data of Scorza et al [36] who used the EMBED program [38,39] at the HF level in combination with second order Møller-Plesset theory for an estimate of the correlation energy.…”
Section: The Neutral and Charged Oxygen Vacancysupporting
Single neutral and positively charged oxygen vacancies (F and F þ centers) in a-Al 2 O 3 are investigated using the supercell model (SCM) at the Hartree-Fock (HF) and density functional theory (DFT) level and the cyclic cluster model (CCM) implemented in the semiempirical MSINDO method. Results of supercell and cyclic cluster calculations for the cohesive energy of the perfect Al 2 O 3 crystal are compared with the experimental value for the heat of atomization. The defect formation energy of the unrelaxed F center is calculated with the SCM. The CCM is used to calculate the defect formation energy of the F and the F þ centers. Relaxation effects for the nearest neighbors (NN) and the nextnearest neighbors (NNN) of the F and F þ centers are investigated. The obtained values are compared to other theoretical literature data.
“…[12,13,14,15,16,17,18]). Several types of embedded cluster techniques have been used successfully to study the structure and properties of defects in ionic oxides, such as MgO (see, for example, [19,20,21,22,23,24]), CaO [25] and SiO 2 [26,27].…”
Abstract. We have studied the structure and spectroscopic properties of the oxygen divacancy defect in Yttrium-stabilized ZrO2 using periodic and embedded cluster methods and GGA and B3LYP density functionals. The results demonstrate that the defect spectroscopic properties depend on the particular arrangement of Y dopants near vacancies. The optical transition energies calculated for the negatively charged state of the divacancy at 2.8 eV and 3.3 eV are in agreement with experimental data. The second set of transitions between 1.9 eV and 2.7 eV corresponds to the electron transfer between vacancies. The calculated EPR g-tensor values are in agreement with other works. The results support the proposed attribution of the optical absorption peaking at 3.3 eV and related EPR spectra to Zr 3+ ions in the YSZ matrix, however, they are not fully conclusive due to dependence on Y concentration.
“…Of course, approximations to the form of the functional are admissible and often necessary. However, additional approximations, which are introduced in many embedding schemes [10][11][12][13][19][20][21]24 during the SCF procedure for determining the ground-state density matrix, may bare a high risk of seriously violating the variational principle. 9…”
Even if an isolated defect results only in a local perturbation of the electron density, the wave function and the first-order reduced density matrix may still exhibit a long-range response to the defect. We present an axiomatic approach to the construction of a general-purpose embedding scheme which is able to cope with this problem. We start from a list of requirements, which we consider pertinent to an accurate embedding technique, and we proceed to demonstrate that the extended subspace approach recently proposed by Head and Silva [J. Chem. Phys. 104, 3244 (1996)] is the minimal realization of such an embedding scheme. The variational principle, strict fulfillment of the Pauli exclusion principle, a finite dimensional parameter space, and the possibility to perform the minimization by a standard SCF (self-consistent field) procedure are the key requirements which lead to a constrained SCF procedure. Self-embedding consistency and local completeness of the Hilbert space can then be realized by a mathematically very simple construction principle for the active subspace which can be formulated independent of any basis set. We analyze the spatial structure of the resulting minimal orbital space by means of tight-binding model Hamiltonians. For metal systems, we find active and frozen constrained SCF spaces to necessarily interlock in a strong and complicated fashion.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.