1971
DOI: 10.1109/tns.1971.4326419
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Vacuum Ultraviolet Radiation Effects in SiO2

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Cited by 183 publications
(32 citation statements)
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“…It is in this region where the band-to-band transitions would be expected to occur by analogy with those from SiO2 ( ,,, 8.8 eV) (Reilly, 1970;Phillip, 1966;and Powell and Derbenwick, 1971); or A1203 (-~ 8.5 eV) (Reilly, 1970;and Ciraci and Batra, 1983).…”
Section: Electronic Absorptionmentioning
confidence: 98%
“…It is in this region where the band-to-band transitions would be expected to occur by analogy with those from SiO2 ( ,,, 8.8 eV) (Reilly, 1970;Phillip, 1966;and Powell and Derbenwick, 1971); or A1203 (-~ 8.5 eV) (Reilly, 1970;and Ciraci and Batra, 1983).…”
Section: Electronic Absorptionmentioning
confidence: 98%
“…5.7. Therefore, the response (in terms of charging) of the collector to the irradiation will be determined by the spectrum of the present imperfections and, in turn, can be used for characterizing the trapping centres (Powell and Derbenwick, 1971). In the case of high-energy radiation like X-rays or γ-radiation, all the components of the emitterÀcollector field-electrode sample structure are sufficiently transparent, allowing one to avoid fabrication of samples with a specially designed optical input.…”
Section: Electronàhole Plasma Generation In the Collectormentioning
confidence: 99%
“…It should be added though that this number may not represent the total number of E 0 type centers inherent to the fumed nanoparticles, as the VUV treatment may not have exhaustively activated all defect sites present due to the small penetration depth ($10 nm) [27] of the VUV photons in SiO 2 in combination with the powder nature of the sample (geometric shadowing). However, most of the precursor sites may have been activated because of the prolonged irradiation treatment with regular intermittent stirring of the fume powder.…”
Section: E 0 Type Centermentioning
confidence: 99%