Nanowires Science and Technology 2010
DOI: 10.5772/39485
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Transition Metal-Doped ZnO Nanowires: En Route Towards Multi-colour Light Sensing and Emission Applications

Abstract: 368and strength of the chemical bonds of wide-band gap semiconductors, photodetectors engineered based on most of metal-oxides can withstand highly elevated T and hostile environments. Despite the fact that carrier mobilities are much smaller in cases of metal oxides compared with those of many conventional semiconductors, owing to the drastically increased dielectric strength of metal oxides, much larger carrier velocities can be readily achieved by applying much higher electric fields/device biases. The prop… Show more

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Cited by 5 publications
(3 citation statements)
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“…2 Moreover, the band-to-band electronic transitions are enhanced by Fe-doping at lattice sites for reducing charge trapping. 15 In the present work, a luminescent Fe-doped ZnO nanowire based oxygen gas sensor has been investigated for fast response/ recovery time. The ZnO nanowires were synthesized by employing an alternative approach using Fe and Zn as starting materials in a controlled environment for the growth of free standing Fe-doped ZnO nanowires in contrast to the catalyst coated substrates used for obtaining ZnO nanowires during a typical vapour phase transport process.…”
Section: Introductionmentioning
confidence: 99%
“…2 Moreover, the band-to-band electronic transitions are enhanced by Fe-doping at lattice sites for reducing charge trapping. 15 In the present work, a luminescent Fe-doped ZnO nanowire based oxygen gas sensor has been investigated for fast response/ recovery time. The ZnO nanowires were synthesized by employing an alternative approach using Fe and Zn as starting materials in a controlled environment for the growth of free standing Fe-doped ZnO nanowires in contrast to the catalyst coated substrates used for obtaining ZnO nanowires during a typical vapour phase transport process.…”
Section: Introductionmentioning
confidence: 99%
“…(1) Также на кривой 1 наблюдается слабое формирование нескольких пиков при энергиях возбуждения 2, 4, 6, 8, 12 и 14 эВ. Основные максимумы в спектрах обозначены буквами А, Б, В, Г и Д. Максимум А при энергии 2.5 эВ в спектре ПТ показывает наличие дорадиационных дефектов (вакансий кислорода в поверхностных слоях ZnO) [17][18][19]. Достаточно большое количество работ посвящено исследованию пика А в образцах нелегированного ZnO, который располагается в области спектра, связанной с собственными дефектами, и имеет максимум около 2.0−2.5 эВ.…”
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“…Далее при энергиях облучения 20 эВ (кривая 3) появляется максимум А при энергии 1.5 эВ, также исчезает максимум Г при энергии 8 эВ. Образование максимумов А при энергии 1.5 эВ на энергетической оси (максимум при 1.5 эВ − вакансии цинка, поверхностная дырка по данным [17]) указывает на то, что начинается образование вакансии цинка. Также исчезновение из спектров ПТ максимума Г при энергии 8 эВ показывает снижение концентрации атомов цинка на границе раздела и доминирование атомов кислорода на поверхности (максимум Д при энергии 12 эВ).…”
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