2012
DOI: 10.1007/s10971-012-2856-x
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Influence of oxygen atmosphere on the photoluminescence properties of sol–gel derived ZrO2 thin films

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Cited by 40 publications
(12 citation statements)
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“…The emission peaks were observed at 389 nm (3.18 eV), 306 nm (4.05 eV), 602 nm (2.05 eV) and 767 nm (1.61 eV). The energy gap of tetragonal ZrO 2 phase is greater than 5.5 eV [1][2][3]. At 243 nm (5.11 eV) excitation a large intensity emission band of 390 nm is produced.…”
Section: Optical Studiesmentioning
confidence: 99%
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“…The emission peaks were observed at 389 nm (3.18 eV), 306 nm (4.05 eV), 602 nm (2.05 eV) and 767 nm (1.61 eV). The energy gap of tetragonal ZrO 2 phase is greater than 5.5 eV [1][2][3]. At 243 nm (5.11 eV) excitation a large intensity emission band of 390 nm is produced.…”
Section: Optical Studiesmentioning
confidence: 99%
“…At 243 nm (5.11 eV) excitation a large intensity emission band of 390 nm is produced. The excitation band at 243 nm corresponds to energy near the energy gap of ZrO 2 tetragonal phase and has been assigned to grain boundaries defect states, which are an inherent aspect of the nanocrystallinity [2][3][4]. The intense zirconia emission peak at E389 nm in the ZrO 2 thin film can be due to the ionized oxygen vacancies (F and F _ centers) from the conduction band.…”
Section: Optical Studiesmentioning
confidence: 99%
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“…Due to its excellent optical properties, such as high refractive index, large optical band gap, low optical loss and high transparency in the visible and near infrared region [3,4], it is widely used as an essential material in the optical fields including broadband interference filters and active electro-optical devices. ZrO 2 is an ideal host material for various phosphors, because of its wide band-gap and low phonon energy [5].…”
Section: Introductionmentioning
confidence: 99%