2019
DOI: 10.1016/j.jlumin.2018.11.043
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A study of 8 MeV e-beam on localized defect states in ZnO nanostructures and its role on photoluminescence and third harmonic generation

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Cited by 29 publications
(18 citation statements)
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“…ZnO has attracted the attention of many researchers for many years due to some of its properties such as wide band gap (3.30eV), high exciton binding energy (60MeV) at room temperature, stable hexagonal wurtzite structure with space group P63mc [1,2]. These features have made it desirable for several applications including photocatalysis [3], surface acoustic wave devices [4], photodetectors [5], gas sensors [6], light-emitting diodes [7,8], and solar cells [9].…”
Section: Introductionmentioning
confidence: 99%
“…ZnO has attracted the attention of many researchers for many years due to some of its properties such as wide band gap (3.30eV), high exciton binding energy (60MeV) at room temperature, stable hexagonal wurtzite structure with space group P63mc [1,2]. These features have made it desirable for several applications including photocatalysis [3], surface acoustic wave devices [4], photodetectors [5], gas sensors [6], light-emitting diodes [7,8], and solar cells [9].…”
Section: Introductionmentioning
confidence: 99%
“…Raman spectroscopy is a nondestructive tool that has been widely used for studying phonon dynamics, structure, and the phases of different materials, including nanostructured materials. [1][2][3][4][5][6][7][8] In the first-order Raman scattering process, when long-range order exists over length scales comparable with the wavelength of the incident photons, only phonons with small wave vectors (i.e., those near the Brillouin-zone center) contribute to the Raman signal, producing Stokes lines with approximately Lorentzian shape and narrow full width at half maximum (FWHM). [9,10] In the case of nanomaterials, where long-range order is reduced to submicron or nanometric dimensions, the wave vector selection rule is relaxed, allowing phonons further away from the Brillouin-zone center to contribute to the Raman signal.…”
Section: Introductionmentioning
confidence: 99%
“…[9,10,[12][13][14] Confinement effects have been observed in structurally modified single crystals and polycrystals. [5,6,[15][16][17] Ionizing radiation, for example, can produce disorder in a crystal through the introduction of defects such as ion tracks, voids, phase precipitates, and dislocations. [18,19] When disorder is introduced, the correlation length of the phonons is reduced as the wave vector selection rule is relaxed.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, high energies of electrons or gamma rays (more than 1-5 MeV) lead to the formation of electronic cascades in the structure, which can lead to a significant change in the electron density of nanostructures, which leads to ordering of the structure and a change in the orientation of texture planes. At the same time, when irradiated with electronic and gamma radiation, the probability of an increase in the geometric dimensions of nanostructures is extremely small, which indicates the great promise of these types of radiation for directional modification and reduction of the disequilibrium of structural parameters in nanomaterials [16][17][18][19][20]. The absence of oxidation processes as a result of phase transformations upon irradiation with electrons or gamma rays opens up wide possibilities for using these types of radiation for the directed modification of iron-nickel or iron-containing nanostructures, for which oxidation processes are accompanied by phase transformations and changes in properties [21][22][23][24][25].…”
Section: Introductionmentioning
confidence: 99%