Quantum chemical modeling of photoabsorption and photoluminescence of the [AlO4]0 defect in bulk SiO2

Structures, vertical excitation, and photoluminescence energies of the eight lowest electronic states of the [AlO4]0 defect in bulk SiO2 have been calculated using the complete active space self-consistent field, equation-of-motion coupled cluster, outer valence Green functions, and multireference configuration interaction methods within a cluster approximation. Two groups of electronic states with different types of the hole localization on oxygen atoms have been found. In two lower states the unpaired electron is localized on a single O atom, while in the higher energy states this electron is redistributed among two or three O atoms. The excitations to the second group of electronic states are accomplished by photoabsorption in the visible range, whereas photoluminescence energies lie in the infrared region due to significant Stokes shifts.

[1]  Karl Hess,et al.  Magnitude of the threshold energy for hot electron damage in metal–oxide–semiconductor field effect transistors by hydrogen desorption , 1999 .

[2]  Di Pomponio A,et al.  All-electron study of the electronic properties of quartz with Al substitutional impurity. , 1996, Physical review. B, Condensed matter.

[3]  P. Knowles,et al.  An efficient method for the evaluation of coupling coefficients in configuration interaction calculations , 1988 .

[4]  A. S. Zyubin,et al.  Performance of time‐dependent density functional and Green functions methods for calculations of excitation energies in radicals and for Rydberg electronic states , 2003, J. Comput. Chem..

[5]  Bonnie Berger,et al.  Local topology of silica networks , 1998 .

[6]  Michel Dupuis,et al.  Ab initio self-consistent-field molecular orbital calculations on defects associated with radiation damage in alpha quartz , 1991 .

[7]  P. Knowles,et al.  An efficient internally contracted multiconfiguration–reference configuration interaction method , 1988 .

[8]  Joel J. Martin,et al.  Radiation effects in crystalline SiO2: The role of aluminum , 1981 .

[9]  Y. Le Page,et al.  Parameter variation in low-quartz between 94 and 298K , 1980 .

[10]  A. I. Boldyrev,et al.  The upper ionization potentials of F−, LiF−2, BeF−3, BO−2, AlO−2, and NO−3 ions calculated by Green’s function method , 1990 .

[11]  K. Stokbro,et al.  Local chemistry of Al and P impurities in silica , 2000 .

[12]  K. Morokuma,et al.  A NEW ONIOM IMPLEMENTATION IN GAUSSIAN98. PART I. THE CALCULATION OF ENERGIES, GRADIENTS, VIBRATIONAL FREQUENCIES AND ELECTRIC FIELD DERIVATIVES , 1999 .

[13]  John F. Stanton,et al.  The equation of motion coupled‐cluster method. A systematic biorthogonal approach to molecular excitation energies, transition probabilities, and excited state properties , 1993 .

[14]  Yit‐Tsong Chen,et al.  Red and near-infrared photoluminescence from silica-based nanoscale materials: Experimental investigation and quantum-chemical modeling , 2002 .

[15]  Phonon-assisted tunneling and interface quality in nanocrystalline Si/amorphous SiO2 superlattices , 1999 .

[16]  P. Knowles,et al.  An efficient second-order MC SCF method for long configuration expansions , 1985 .

[17]  J. V. Ortiz Electron binding energies of anionic alkali metal atoms from partial fourth order electron propagator theory calculations , 1988 .

[18]  J. Stewart Optimization of parameters for semiempirical methods I. Method , 1989 .

[19]  G. Pacchioni,et al.  Ab initio theory of optical transitions of point defects in SiO 2 , 1998 .

[20]  J. Mackey EPR Study of Impurity‐Related Color Centers in Germanium‐Doped Quartz , 1963 .

[21]  A. D. Corso,et al.  Microscopic structure of the substitutional Al defect in α quartz , 2000 .

[22]  M. Martini,et al.  ROLE OF [ALO4](0) CENTERS IN THE 380-NM THERMOLUMINESCENCE OF QUARTZ , 1995 .

[23]  Lorenz S. Cederbaum,et al.  Computational methods for the one-particle green's function , 1984 .

[24]  G. Pacchioni,et al.  Theoretical description of hole localization in a quartz Al center: The importance of exact electron exchange , 2000 .

[25]  Philippe M. Fauchet,et al.  Ordering and self-organization in nanocrystalline silicon , 2000, Nature.

[26]  L. Skuja Optically active oxygen-deficiency-related centers in amorphous silicon dioxide , 1998 .

[27]  P. Knowles,et al.  A second order multiconfiguration SCF procedure with optimum convergence , 1985 .

[28]  L. Cederbaum,et al.  Many-body calculation of electron affinities: C2 and a prediction for P2 , 1977 .

[29]  Dennis R. Salahub,et al.  Molecular excitation energies to high-lying bound states from time-dependent density-functional response theory: Characterization and correction of the time-dependent local density approximation ionization threshold , 1998 .

[30]  L. D. Negro,et al.  Optical gain in silicon nanocrystals , 2000, Nature.

[31]  M. O'brien The structure of the colour centres in smoky quartz , 1955, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[32]  K. Raghavachari,et al.  Optical properties of point defects in SiO2 from time-dependent density functional theory , 2002 .