1987
DOI: 10.1103/physrevb.35.8223
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Oxygen vacancy and theE1center in crystallineSiO2

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Cited by 305 publications
(130 citation statements)
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“…292,293 For a covalent material like silica, bond cutting brings about the formation of a variety of surface defects, the most relevant being: the Q 3 (•) silyl Si• , the Q 3 (O•) siloxy E' SiO•, the Q 2 (:) >Si: and the Q 2 (O) silanone >Si=O. The nature and stability of these defects has been discussed in the literature [69][70][71][294][295][296][297][298][299][300][301][302][303][304][305] showing that all of them, without exception, are thermodynamically unstable with respect to water hydroxylation. As water is ubiquitously present during biomolecules adsorption these defects should not play an important role in that case.…”
Section: The Periodic Boundary Conditions Approachmentioning
confidence: 99%
“…292,293 For a covalent material like silica, bond cutting brings about the formation of a variety of surface defects, the most relevant being: the Q 3 (•) silyl Si• , the Q 3 (O•) siloxy E' SiO•, the Q 2 (:) >Si: and the Q 2 (O) silanone >Si=O. The nature and stability of these defects has been discussed in the literature [69][70][71][294][295][296][297][298][299][300][301][302][303][304][305] showing that all of them, without exception, are thermodynamically unstable with respect to water hydroxylation. As water is ubiquitously present during biomolecules adsorption these defects should not play an important role in that case.…”
Section: The Periodic Boundary Conditions Approachmentioning
confidence: 99%
“…These initial calculations were motivated by the experimental evidence suggesting that the excited state has the structure of a close oxygen-oxygen p i r or peroxy linkage associated with a nearby oxygen vacancy; this evidence includes the similarity of the large uniaxial fine structure to the fine structure of molecular oxygen (Tinkham and Strandberg 1954) and the resemblance of the 5.4 eV a.bsorption line to the 5.8 eV absorption in the oxygen vacancy or E-centre which has been known in quartz for some years (Tanimura et a1 1983, Weeks 1956, Rudra and Fowler 1987. We have reported elsewhere (Fisher et a1 1989, Fisher 1989) some of our calcuhtions designed to test this model; in particular, we found that the fine structure to be expected from an (O,),-molecular ion is similar to that observed in quartz if the interatomic axis is identified with the fine-structure principal axis.…”
Section: Semi-empirical Calculations and The Peroxy Modelmentioning
confidence: 99%
“…4) E' γ centers have long spin-lattice relation times (T 1 ) of ≈200 µs at room temperature [29,30]. There are many variations of E' γ centers found in amorphous SiO 2 due to the large spread of bond angles and bond lengths found in the amorphous network [31][32][33][34][35]. While the microscopic theory for the E' γ center is not without controversy [36], the common feature among all variations is an unpaired electron on a silicon atom back-bonded to three oxygen atoms, i.e.…”
Section: Properties Of Suitable Paramagnetic Electronic Statesmentioning
confidence: 99%