2017
DOI: 10.1016/j.physe.2017.01.009
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Effect of growth time on Ti-doped ZnO nanorods prepared by low-temperature chemical bath deposition

Abstract: Ti-doped ZnO nanorod arrays were grown onto Si substrate using chemical bath deposition (CBD) method at 93 °C. To investigate the effect of time deposition on the morphological, and structural properties, four Ti-doped ZnO samples were prepared at various deposition periods of time (2, 3.5, 5, and 6.5 h). FESEM images displayed high-quality and uniform nanorods with a mean length strongly dependent upon deposition time; i.e. it increases for prolonged growth time. Additionally, EFTEM images reveal a strong ero… Show more

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Cited by 51 publications
(22 citation statements)
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“…The axial growth rate was found to be more pronounced than the lateral growth rate, which can be attributed to the low surface free energy within the c-axis [31,32]. Figure 6 shows that the length-growth rate (length/time) increases first then drops as the deposition time increases, which is associated with the consumption of the (Zn +2 , OH −1 ) species with time; similar results have been reported previously [25,33]. The morphological parameters are listed in table 3.…”
Section: Resultssupporting
confidence: 83%
See 1 more Smart Citation
“…The axial growth rate was found to be more pronounced than the lateral growth rate, which can be attributed to the low surface free energy within the c-axis [31,32]. Figure 6 shows that the length-growth rate (length/time) increases first then drops as the deposition time increases, which is associated with the consumption of the (Zn +2 , OH −1 ) species with time; similar results have been reported previously [25,33]. The morphological parameters are listed in table 3.…”
Section: Resultssupporting
confidence: 83%
“…Figure 9 shows that the Schottky LED with 1.2-μm ZnO NRs has 10 times higher emission intensity than that of one with 0.383-μm ZnO NRs and that the Schottky LED with 3.9-μm ZnO NRs have 300 times higher emission intensity than that of one with 0.383-μm ZnO NRs. It was previously reported that the deep band emission intensity depends on the size of the ZnO and that the extraction factor for ZnO is low due to its high absorption coefficients (∼2×105 cm −1 ), which increases the probability of ultraviolet (UV) reabsorption within the crystal itself [32][33][34]. This reabsorbed UV can excite the defect states in the structures, resulting in visible deep band emission because the defects responsible for this emission are not confined near the surface but are ubiquitous inside the ZnO NRs [29].…”
Section: Resultsmentioning
confidence: 99%
“…As the immersion time increased to 2 h, the length of the ZnO NRs were approximately 1.6 µm which is almost twice longer than 0.5 h sample, which is an improvement with respect to other hydrothermal method that used acetates and nitrates-derived precursor to grow nanorods (the minimal immersion time captured from several works to grow nanorods are presented in Table 1). However, a further increment in the immersion time to 4 h showed insignificant differences in terms of the morphologies and dimensionality of the ZnO NRs, which can be ascribed to the insufficient amount of Zn 2+ ions supplied to the system, hence abrupted the growth of ZnO NRs [31]. These showed that in a hydrothermal, precursor plays a role in supplying Zn 2+ ions to the system in order to completely form ZnO.…”
Section: Methodsmentioning
confidence: 96%
“…The fact that the radius of 4-coordinate Ga 3+ (0.62 Å) and that of In 3+ (0.81 Å) is closer to that of 4-coordinate Zn 2+ (0.74 Å), make it useful as a codopant for ZnO structures [10,11]. Thin film deposition of ZnO can be carried out by various techniques like sputtering [12], pulsed laser deposition [13], microwave assisted synthesis [14], sol-gel [15], ultrasonic spray pyrolysis [16], chemical bath deposition [17], etc. Among these, radio frequency (RF) sputtering is more suitable for high quality and large area deposition.…”
Section: Introductionmentioning
confidence: 99%