In this work we investigate paramagnetic centers in amorphous germania (alpha-GeO2). We provide an analysis of the Fermi contacts and of the g-tensors calculated by first-principles for the E'-Ge, Ge-Ge and Ge forward-oriented (GeFO) configurations. The electron paramagnetic resonance (EPR) parameters calculated for the Ge-Ge configurations, where the unpaired electron is shared between two Ge nearest neighbors, do not support such a model of the E'-Ge*, nor the latter can be simply regarded as an E'-Ge center with a distorted geometry. A fair agreement with the experimental EPR parameters supports the assignment of the Ge(2) center in a-GeO2 to GeFO configurations. Furthermore we show that electronic levels induced in the bandgap by GeFO configurations are considerably deeper (similar to 1 eV) with respect to those related to the E'-Ge centers. (C) 2015 Elsevier B.V. All rights reserved.

Paramagnetic centers in amorphous GeO2

2015

Abstract

In this work we investigate paramagnetic centers in amorphous germania (alpha-GeO2). We provide an analysis of the Fermi contacts and of the g-tensors calculated by first-principles for the E'-Ge, Ge-Ge and Ge forward-oriented (GeFO) configurations. The electron paramagnetic resonance (EPR) parameters calculated for the Ge-Ge configurations, where the unpaired electron is shared between two Ge nearest neighbors, do not support such a model of the E'-Ge*, nor the latter can be simply regarded as an E'-Ge center with a distorted geometry. A fair agreement with the experimental EPR parameters supports the assignment of the Ge(2) center in a-GeO2 to GeFO configurations. Furthermore we show that electronic levels induced in the bandgap by GeFO configurations are considerably deeper (similar to 1 eV) with respect to those related to the E'-Ge centers. (C) 2015 Elsevier B.V. All rights reserved.
2015
Istituto Officina dei Materiali - IOM -
E '-Ge
Ge(2) center
GeO2
EPR
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/311081
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