1,785 research outputs found

    Chemical and Geometric Transformations of MoS2/WS2 Heterostructures by Plasma Treatment

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    abstract: Two-dimensional (2D) transition metal dichalcogenides (TMDCs) like molybdenum disulfide (MoS2) and tungsten disulfide (WS2) are effective components in optoelectronic devices due to their tunable and attractive electric, optical and chemical properties. Combining different 2D TMDCs into either vertical or lateral heterostructures has been pursued to achieve new optical and electronic properties. Chemical treatments have also been pursued to effectively tune the properties of 2D TMDCs. Among many chemical routes that have been studied, plasma treatment is notable for being rapid and versatile. In Wangโ€™s group earlier work, plasma treatment of MoS2 and WS2 resulted in the formation of MoO3 and WO3 nanosheets and nanoscrolls. However, plasma treatment of 2D TMDC heterostructures have not been widely studied. In this dissertation, MoS2/WS2 vertical and lateral heterostructures were grown and treated with air plasma. The result showed that the vertical heterostructure and lateral heterostructures behaved differently. For the vertical heterostructures, the top WS2 layer acts as a shield for the underlying MoS2 monolayer from oxidizing and forming transition metal oxide nanoscrolls, as shown by Raman spectroscopy and atomic force microscopy (AFM). On the contrary, for the lateral heterostructures, the WS2 that was grown surrounding the MoS2 triangular core served as a tight frame to stop the propagation of the oxidized MoS2, resulting a gradient of crack distribution. These findings provide insight into how plasma treatment can affect the formation of oxide in heterostructure, which can have further application in nanoelectronic devices and electrocatalysts.Dissertation/ThesisMasters Thesis Materials Science and Engineering 201

    Study of Surface Morphology and Microstructure of Electrodeposited Polycrystalline Cu Films

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    The applications of polycrystalline films range from interconnects in the electronics and semiconductor industry to solar cells and as corrosion protection. Despite their significance, factors that determine their microstructure and morphology remain largely unsolved. The surface and microstructure of electrodeposited polycrystalline Cu films were investigated. This involves looking at the later growth stages of Cu films using different surface and bulk characterization techniques. The surface evolution of an electrodeposited Cu film was imaged in real-time using a Highspeed Atomic Force Microscope (HS-AFM). This provides details about how the film structure coarsens with time. The high-resolution video showed accelerated local grain growth and grain overgrowth at different locations of the film. A combination of both of these mechanisms could drive structural coarsening. The microstructure could play a role in inducing faster growth in certain grains. How the local and large-scale roughness varies with film thickness is studied by scaling analysis. As a complement to scaling analysis, variation in the local slope with thickness is calculated using slope analysis. Rapid growth was observed in the regions where the HS-AFM tip was scanning. The removal of oxygen adlayer from the surface by the tip could promote faster growth in these regions. Pulsed electrodeposition produced Cu films with hexagonal structures. They are known to be twinned which is a desirable feature in applications that require superior mechanical and electrical properties. The effect of electrode potential on grain size was studied. Using a watershed segmentation algorithm, the grain area was calculated from the AFM images. The grain area showed an increasing trend with increasing overpotential. Slope analysis on the โ€™hexagonsโ€™ and the complete films electrodeposited at higher potential revealed higher slopes and distinct slope distribution. Cross-sectional Focused Ion Beam (FIB) milling confirmed that horizontal twins are present in the pulse-deposited Cu films. The hexagonal pyramids with twins could be produced by one of the two mechanisms, stress relaxation during the โ€™OFFโ€™ period of pulsing or driven by screw dislocation. We attribute the origin of the hexagons to spiralling screw dislocations. A template matching algorithm was developed to try and correlate the surface and microstructural data of a Cu film grown on a microelectrode. It involved matching the AFM and Electron Back Scatter Diffraction (EBSD) data on the later FIB milled sample, thus relating surface topography to crystallographic orientation. The crystallographic orientation of the edge of the microelectrode and its centre showed different orientations, switching from (111) to (110). Twinning was investigated at the edge and the centre of the microelectrode revealing the presence of stacking fault twins in both of these regions

    Lead Free CH3NH3SNI3 Perovskite Thin-Film with P-type Semiconducting Nature and Metal-like Conductivity

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    CH3NH3SnI3 and CH3NH3PbI3 have become very promising light absorbing materials for photovoltaic devices over the last several years. CH3NH3PbI3 based perovskite solar cells have reached a solar-to-electricity conversion efficiency of ~ 22%. Nevertheless, CH3NH3PbI3 perovskite solar cells contain lead, which has serious consequences for the environment and human health. In this work, the lead was replaced with less toxic tin. Lead free CH3NH3SnI3 perovskite thin film was prepared by two low temperature solution processing methods and characterized using various tools such as Xray Diffraction (XRD) and absorption spectroscopy (UV-VIS). The distinctive p-type semiconducting nature and metal like conductivity of CH3NH3SnI3 were confirmed by the measurements of electrical and optical properties. Crystal structures and uniform film formation of CH3NH3SnI3 layer were analyzed by XRD and scanning electron microscopy (SEM). The CH3NH3SnI3 film morphology, uniformity, light absorption and electrical properties strongly depend on the preparation methods and precursor solutions. The CH3NH3SnI3 perovskites fabricated using dimethylformamide (DMF) exhibited higher crystallinity and stronger light harvesting capability than those fabricated using a blend solvent of dimethyl sulfoxide (DMSO) and gamma-butyrolactone (GBL). The local nanoscale photocurrent mapping confirmed that CH3NH3SnI3 can be used as an active layer and has a potential to fabricate lead free photovoltaic devices. The CH3NH3SnI3 film also showed a strong absorption in visible and near infrared spectrum with an absorption onset of 1.3 eV

    ๋ณ€ํ˜•๋œ ์ด์ข…๊ตฌ์กฐ ์‚ฐํ™”๋ฌผ ๋‚˜๋…ธ ๊ฒฐ์ •์˜ ์„ฑ์žฅ, ์›์ž ๊ตฌ์กฐ ๋ฐ ์ด‰๋งค ํŠน์„ฑ์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€(์—๋„ˆ์ง€ํ™˜๊ฒฝ ํ™”ํ•™์œตํ•ฉ๊ธฐ์ˆ ์ „๊ณต), 2020. 8. ํ˜„ํƒํ™˜.Strain engineering of the inorganic nanocrystal is a promising approach necessary to address emerging global energy, resource, and environmental issues. When different materials are combined to produce heterostructured nanocrystal, the epitaxially-strained lattices can be formed at the heterointerface. In particular, the strain effect at the nanoscale can alter the surface lattice spacing and tune the electronic structure of the surface atoms, thus modifying the catalytic activity. The strain can be tuned by a lattice mismatch between the substrate and the overgrowth phase with a different crystal structure or crystallographic orientation. The strain engineering has been developed in heterostructured nanocrystals with different material combinations, including metals, semiconductors, and oxides. However, studies on the strained structure in oxide nanocrystals are limited because the synthesis of such structures has not been well established. In this thesis, I have designed and synthesized a model system that could investigate the strain effect on the regulation of the surface electronic structure for the design of better catalysts. The strained heterostructured oxide nanocrystals were produced using seed-mediated growth. The unique structure of these nanocrystals has been successfully studied with electron microscopy. The first part of this thesis is an overview of epitaxial growth in thin-film technology and its analogy to three-dimensional (3D) polyhedral epitaxial growth. Chapter 2 describes the design principles for producing highly ordered multigrain nanostructures. Identification of the principles was achieved by synthesizing the nanocrystals with misfit-strain-induced uniform grain boundary defects, imaging the deformed structure at the nanometer scale using a scanning transmission electron microscopy (STEM), and measuring the strain field. The seed-mediated approach was used to grow Mn3O4 grains on a cubic Co3O4ยฌ nanocrystal core. The facets of the cube nanocrystal substrates can guide the growth direction of the shell, creating a gap between the lattices of the adjacent Mn3O4 grains. Unlike the previous studies on the heteroepitaxial strains, the grain boundary (GB) defects in this new multigrain nanocrystal were induced by the geometric misfit strain between the adjacent Mn3O4 grains. Since the defects occur along the edges of the core, a uniform core shape is a prerequisite for achieving uniform GB defects. The strain tensor near the GB lattices reveals that the Mn3O4 shell accommodates a large epitaxial strain per GB without dislocation. Chapter 3 presents the epitaxially strained CeO2/Mn3O4 nanocrystals for antioxidant applications. The Mn3O4 lattices are highly strained due to the large lattice mismatch between CeO2 and Mn3O4. The heterostructured nanocrystals with different compositions were prepared to study the strain effect by comparing the surface oxygen vacancy and the characteristics of surface reducibility. Due to the enhanced ability to scavenge the reactive oxygen species (ROS), the nanocrystal with strained Mn3O4 layer can protect the hematopoietic intestinal stem cells from irradiation.๋ฌด๊ธฐ ๋‚˜๋…ธ ๊ฒฐ์ •์˜ ๋ณ€ํ˜• ์—”์ง€๋‹ˆ์–ด๋ง์€ ์—๋„ˆ์ง€, ์ž์› ๋ฐ ํ™˜๊ฒฝ๊ณผ ๊ฐ™์€ ์ „ ์ง€๊ตฌ์ ์ธ ๋ฌธ์ œ๋ฅผ ํ•ด๊ฒฐํ•˜๋Š” ๋ฐ ํ•„์š”ํ•œ ์œ ๋งํ•œ ์ ‘๊ทผ๋ฒ•์ด๋‹ค. ์„œ๋กœ ๋‹ค๋ฅธ ์žฌ๋ฃŒ๋ฅผ ์กฐํ•ฉํ•˜์—ฌ ์ด์ข… ๊ตฌ์กฐํ™”๋œ ๋‚˜๋…ธ ๊ฒฐ์ •์„ ์ƒ์„ฑํ•  ๋•Œ, ์—ํ”ผํƒ์…œ ๋ณ€ํ˜•๋œ ๊ฒฉ์ž๋Š” ์ด์ข… ๊ณ„๋ฉด์— ํ˜•์„ฑ๋  ์ˆ˜ ์žˆ๋‹ค. ํŠนํžˆ, ๋‚˜๋…ธ ๊ทœ๋ชจ์—์„œ์˜ ๋ณ€ํ˜• ํšจ๊ณผ๋Š” ํ‘œ๋ฉด์˜ ๊ฒฉ์ž ๊ฐ„๊ฒฉ์„ ๋ณ€๊ฒฝํ•˜๊ณ  ํ‘œ๋ฉด ์›์ž์˜ ์ „์ž ๊ตฌ์กฐ๋ฅผ ์กฐ์ •ํ•˜์—ฌ, ์ด‰๋งค ํ™œ์„ฑ์„ ๋ณ€ํ˜•์‹œํ‚ฌ ์ˆ˜ ์žˆ๋‹ค. ๋ณ€ํ˜•์€ ์ƒ์ดํ•œ ๊ฒฐ์ • ๊ตฌ์กฐ๋‚˜ ๊ฒฐ์ •ํ•™์  ๋ฐฐํ–ฅ์˜ ๊ธฐํŒ๊ณผ ์ฆ์ฐฉ์ƒ ์‚ฌ์ด์˜ ๊ฒฉ์ž ๋ถ€์ •ํ•ฉ์— ์˜ํ•ด ์กฐ์ •๋œ๋‹ค. ๋ณ€ํ˜• ์—”์ง€๋‹ˆ์–ด๋ง์€ ๊ธˆ์†, ๋ฐ˜๋„์ฒด ๋ฐ ์‚ฐํ™”๋ฌผ์„ ํฌํ•จํ•œ ๋‹ค์–‘ํ•œ ์žฌ๋ฃŒ ์กฐํ•ฉ๋œ ์ด์ข…๊ตฌ์กฐ ๋‚˜๋…ธ ๊ฒฐ์ •์—์„œ ๊ฐœ๋ฐœ๋˜์–ด ์™”๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์‚ฐํ™”๋ฌผ ๋‚˜๋…ธ ๊ฒฐ์ •์—์„œ์˜ ๋ณ€ํ˜• ๊ตฌ์กฐ์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋Š” ์ด๋Ÿฌํ•œ ๊ตฌ์กฐ์˜ ํ•ฉ์„ฑ๋ฒ•์ด ์ž˜ ํ™•๋ฆฝ๋˜์ง€ ์•Š์•˜๊ธฐ ๋•Œ๋ฌธ์— ์ œํ•œ์ ์ด๋‹ค. ์ด ๋…ผ๋ฌธ์—์„œ, ๋” ๋‚˜์€ ์ด‰๋งค์˜ ์„ค๊ณ„๋ฅผ ์œ„ํ•˜์—ฌ ํ‘œ๋ฉด์˜ ์ „์ž ๊ตฌ์กฐ ์กฐ์ ˆ์— ๋Œ€ํ•œ ๋ณ€ํ˜• ํšจ๊ณผ๋ฅผ ์—ฐ๊ตฌํ•  ์ˆ˜ ์žˆ๋Š” ๋ชจ๋ธ ์‹œ์Šคํ…œ์„ ์„ค๊ณ„ํ•˜๊ณ  ํ•ฉ์„ฑํ–ˆ๋‹ค. ๋ณ€ํ˜•๋œ ์ด์ข…๊ตฌ์กฐ ์‚ฐํ™”๋ฌผ ๋‚˜๋…ธ ๊ฒฐ์ •์€ ์ข…์ž ๋งค๊ฐœ ์„ฑ์žฅ์„ ์‚ฌ์šฉํ•˜์—ฌ ์ œ์กฐ๋˜์—ˆ๋‹ค. ์ด๋Ÿฌํ•œ ๋‚˜๋…ธ ๊ฒฐ์ •์˜ ๋…ํŠนํ•œ ๊ตฌ์กฐ๋Š” ์ „์ž ํ˜„๋ฏธ๊ฒฝ์œผ๋กœ ์„ฑ๊ณต์ ์œผ๋กœ ์—ฐ๊ตฌ๋˜์—ˆ๋‹ค. ์ด ๋…ผ๋ฌธ์˜ 1์žฅ์€ 2์ฐจ์› ๋ฐ•๋ง‰ ๊ธฐ์ˆ ์˜ ์—ํ”ผํƒ์…œ ์„ฑ์žฅ๊ณผ 3 ์ฐจ์› ๋‹ค๋ฉด์ฒด์™€์˜ ์œ ์‚ฌ์„ฑ์— ๋Œ€ํ•œ ๊ฐœ์š”์ด๋‹ค. 2 ์žฅ์€ ๊ณ ๋„๋กœ ์ •๋ˆ๋œ ๋ฉ€ํ‹ฐ ๊ทธ๋ ˆ์ธ ๋‚˜๋…ธ ๊ตฌ์กฐ๋ฅผ ์ƒ์„ฑํ•˜๊ธฐ ์œ„ํ•œ ์„ค๊ณ„ ์›๋ฆฌ๋ฅผ ์„ค๋ช…ํ•œ๋‹ค. ์›๋ฆฌ ๋ฐœ๊ฒฌ์€ ๋ถ€์ •ํ•ฉ ๋ณ€ํ˜•์ด ์œ ๋ฐœ๋œ ๊ท ์ผํ•œ ๊ฒฝ๊ณ„ ๊ฒฐํ•จ์œผ๋กœ ๋‚˜๋…ธ ๊ฒฐ์ •์„ ํ•ฉ์„ฑํ•˜๊ณ , ์ฃผ์‚ฌ ํˆฌ๊ณผ ์ „์ž ํ˜„๋ฏธ๊ฒฝ์„ ์‚ฌ์šฉํ•˜์—ฌ ๋‚˜๋…ธ ๋ฏธํ„ฐ ์Šค์ผ€์ผ์—์„œ ๋ณ€ํ˜•๋œ ๊ตฌ์กฐ๋ฅผ ์ด๋ฏธ์ง•ํ•˜๊ณ , ๋ณ€ํ˜• ์žฅ์„ ์ธก์ •ํ•จ์œผ๋กœ์จ ๋‹ฌ์„ฑ๋˜์—ˆ๋‹ค. ์‹œ๋“œ ๋งค๊ฐœ ์ ‘๊ทผ๋ฒ•์„ ์‚ฌ์šฉํ•˜์—ฌ ์ž…๋ฐฉํ˜• Co3O4 ๊ฒฐ์ • ์ฝ”์–ด์—์„œ Mn3O4 ์ž…์ž๋ฅผ ์„ฑ์žฅ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋‹ค. ๊ธฐํŒ์ธ ์ž…๋ฐฉ์ฒด ๋‚˜๋…ธ ๊ฒฐ์ •์˜ ๋ฉด์€ ์‰˜์˜ ์„ฑ์žฅ ๋ฐฉํ–ฅ์„ ์•ˆ๋‚ด ํ•  ์ˆ˜ ์žˆ๊ณ , ์ธ์ ‘ํ•œ Mn3O4 ์ž…์ž์˜ ๊ฒฉ์ž ์‚ฌ์ด์— ํ‹ˆ์„ ์ƒ์„ฑํ•œ๋‹ค. ์ด์ข… ์—ํ”ผํƒ์…œ ๋ณ€ํ˜•์— ๋Œ€ํ•œ ์ด์ „์˜ ์—ฐ๊ตฌ์™€๋Š” ๋‹ฌ๋ฆฌ, ์ด ์ƒˆ๋กœ์šด ๋‹ค๊ฒฐ์ • ๋‚˜๋…ธ ๊ฒฐ์ •์—์„œ์˜ ์ž…์ž ๊ฒฝ๊ณ„ ๊ฒฐํ•จ์€ ์ธ์ ‘ํ•œ Mn3O4 ์ž…์ž ์‚ฌ์ด์˜ ๊ธฐํ•˜ํ•™์  ๋ถ€์ •ํ•ฉ ๋ณ€ํ˜•์— ์˜ํ•ด ์œ ๋ฐœ๋˜์—ˆ๋‹ค. ๊ฒฐํ•จ์€ ์ฝ”์–ด์˜ ๊ฐ€์žฅ์ž๋ฆฌ๋ฅผ ๋”ฐ๋ผ ๋ฐœ์ƒํ•˜๊ธฐ ๋–„๋ฌธ์— ๊ท ์ผํ•œ ๊ฒฝ๊ณ„ ๊ฒฐํ•จ์„ ๋‹ฌ์„ฑํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ๊ท ์ผํ•œ ํ˜•์ƒ์˜ ์ฝ”์–ด๊ฐ€ ์ „์ œ ์กฐ๊ฑด์ด๋‹ค. ๊ฒฝ๊ณ„ ๊ฒฐํ•จ ๊ฒฉ์ž ๊ทผ์ฒ˜์˜ ๋ณ€ํ˜• ํ…์„œ๋Š” Mn3O4 ์‰˜์ด ์ „์œ„ ์—†์ด ๊ฒฝ๊ณ„ ๊ฒฐํ•จ ๋‹น ํฐ ์—ํ”ผํƒ์…œ ๋ณ€ํ˜•์„ ์ˆ˜์šฉํ•œ๋‹ค๋Š” ๊ฒƒ์„ ๋ณด์—ฌ์ค€๋‹ค. 3 ์žฅ์—์„œ๋Š” ํ•ญ์‚ฐํ™”์ œ ์ ์šฉ์„ ์œ„ํ•œ ์—ํ”ผํƒ์…œ ๋ณ€ํ˜•๋œ CeO2/Mn3O4 ๋‚˜๋…ธ ๊ฒฐ์ •์„ ์ œ์‹œํ•œ๋‹ค. Mn3O4 ๊ฒฉ์ž๋Š” CeO2์™€ Mn3O4 ์‚ฌ์ด์˜ ํฐ ๊ฒฉ์ž ๋ถ€์ •ํ•ฉ์œผ๋กœ ์ธํ•ด ์ƒ๋‹นํžˆ ๋ณ€ํ˜•๋œ๋‹ค. ์ƒ์ดํ•œ ์กฐ์„ฑ์„ ๊ฐ–๋Š” ์ด์ข… ๊ตฌ์กฐํ™”๋œ ๋‚˜๋…ธ ๊ฒฐ์ •์„ ์ œ์กฐํ•˜์—ฌ ํ‘œ๋ฉด ์‚ฐ์†Œ ๊ณต๊ทน ๋ฐ ํ‘œ๋ฉด ํ™˜์› ํŠน์„ฑ์— ๋Œ€ํ•œ ๋ณ€ํ˜• ํšจ๊ณผ๋ฅผ ๋น„๊ต, ์—ฐ๊ตฌํ•˜์˜€๋‹ค. ํ–ฅ์ƒ๋œ ํ™œ์„ฑ์‚ฐ์†Œ ์ œ๊ฑฐ ๋Šฅ๋ ฅ์„ ๋‚˜ํƒ€๋‚ด๋Š” ๋ณ€ํ˜•๋œ Mn3O4 ์ธต์„ ๊ฐ–๋Š” ๋‚˜๋…ธ ๊ฒฐ์ •์„ ์ด์šฉํ•˜์—ฌ ์กฐํ˜ˆ์žฅ ์ค„๊ธฐ ์„ธํฌ๋ฅผ ๋ฐฉ์‚ฌ์„  ์กฐ์‚ฌ๋กœ๋ถ€ํ„ฐ ๋ณดํ˜ธํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค.Chapter 1 Introduction: Synthetic Methods for Epitaxially Strained Heterostructured Nanocrystals .........................1 1.1 Thin-film epitaxy in nanomaterials .......................................................1 1.1.1 Thin-film deposition techniques .................................................1 1.1.2 Growth modes ............................................................................4 1.2 Strain engineering ...............................................................................13 1.2.1 Synthesis of heterostructured nanocrystals ...............................13 1.2.2 Strain in heterostructured nanocrystals .....................................19 1.2.3 Characterization of strained nanocrystals for catalysis .............28 1.3 Dissertation Overview ........................................................................35 1.4 References ...........................................................................................38 Chapter 2 Design and Synthesis of Multigrain Nanocrystals via Geometric Misfit Strain ..................................................44 2.1 Introduction .........................................................................................44 2.2 Experimental Section ..........................................................................46 2.3 Result and Discussion .........................................................................52 2.4 Conclusion ........................................................................................130 2.5 References .........................................................................................131 Chapter 3 Epitaxially Strained CeO2/Mn3O4 Nanocrystals as an Enhanced Antioxidant for Radioprotection ...........137 3.1 Introduction .......................................................................................137 3.2 Experimental Section ........................................................................139 3.3 Result and Discussion .......................................................................145 3.4 Conclusion ........................................................................................176 3.5 References .........................................................................................177 ๊ตญ๋ฌธ ์ดˆ๋ก (Abstract in Korean) ..........................................182Docto

    Caracterizaciรณn estructural y funcional de pelรญculas delgadas nanoporosas mediante microscopรญas electrรณnicas de transmisiรณnbarrido y espectroscopรญas รณpticas

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    Nano-structuration of materials at the mesoscale to give rise to porosity-controlled coatings represents an important breakthrough in the area of Materials Science and Engineering, offering new and enhanced functionalities of interest in fields such as optics, optronics and optoelectronics. In order to optimize their performances, in-depth analyses are required: local information about the morphology, composition and atomic structure, the compactness distribution, but also layer homogeneity, interface and interpenetration between stacked layers or oxidation are extremely important factors that can ruin their way of operation. In this particular context, the objective of the present PhD Thesis is to make significant contributions to the study and development of multifunctional porous nanostructured systems, from their design and elaboration, to the maximum knowledge of their structure and properties, through advanced (S)TEM methods, including 3D reconstructions, elemental analyses at the nanoscale and atomic-scale imaging, combined with optical spectroscopy techniques. In the first instance, given the great potential of the slanted nanostructures generated by means of oblique angle depositions, in which the refractive index gradient can be tuned by the columns tilt and density imposed via the growth angles and parameters, OAD broadband antireflective coatings based on Si, Ge or SiO2 OAD films have been designed, manufactured, and extensively characterized with the aim of maximizing the performance of the optical elements in the vis-IR wavelength range. This same approach has also been implemented to enhance the antireflective capabilities of transparent conductive ITO thin films in the near-IR window without compromising too much their electrical response. On the other hand, the advanced structural and functional characterization of porosity-controlled GaN NW arrays grown by plasma-assisted MBE through (S)TEM methods and vis-IR SE elliposmetry, has helped not only to improve growth processes but also to optimize their resulting optical and electrical properties. Finally, the knowledge and methodologies acquired during the study and optimization of the previous porous systems have been transferred to the development of a two-step procedure, based on the deposition and the subsequent fast oxidation of vanadium-based OAD films in open air atmosphere, for the synthesis of thermochromic VO2 coatings of tunable metal-to-insulator response and controlled grain sizes and crystallinities

    Development and analyses of innovative thin films for photovoltaic applications

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    In solar cell current research, innovative solutions and materials are continuously requested for efficiency improvements. Si-based technology rules over 95% of the market, with silicon heterojunction (SHJ) solar cell reaching 26.7% record efficiency. Nonetheless, hydrogenated amorphous silicon (a-Si:H) layers employed in the structure still have challenges, resolvable with oxygen/nitrogen inclusion. In parallel, new technologies based on different materials still lack in the market due to stability issues or low efficiencies. However, a preliminary study of their properties creates a deeper knowledge exploitable in photovoltaic application. In this perspective, we investigated both innovative Si-based materials (nanocrystalline and amorphous silicon oxy-nitride and oxide thin films, nc-SiOxNy, a-SiOxNy and a-SiOx, respectively) and innovative materials (perovskite lanthanum-vanadium oxide LaVO3 thin films, indium gallium nitride InxGa1-xN and aluminium indium gallium nitride AlxInyGa1-x-yN layers) for solar cell concepts. Different deposition conditions have been employed to extract their influence on compositional, optical, and electrical properties. The study on nc-SiOxNy layers by conductive atomic force microscopy (c-AFM) and surface photovoltage (SPV) has allowed to clarify O, N, and B content, and annealing treatment role on microscopic transport properties. On a-SiOx and a-SiOxNy layers, by spectral ellipsometry, Fourier transform infrared spectroscopy, photoconductance decay and SPV, we can conclude that moderate insertions of O/N in a-Si:H lead to a decrease of optical parasitic absorption, preserving the passivation quality of the layers. The measurements by AFM and Kelvin probe force microscopy on LaVO3 have clearly shown that it is a poor charge-transport medium, thus not suitable for photovoltaic applications. The analysis on InGaN and AlGaInN by SPV measurements has shown how low In content, Si doping and no misfit dislocations in InGaN/GaN structure cause less recombination processes at the interface, whereas, the strain relaxation (tensile and compressive) with the formation of pinholes produces better interfaces in the AlGaInN/GaN samples

    Influence of the substrate-induced strain and irradiation disorder on the Peierls transition in TTF-TCNQ microdomains

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    The influence of the combined effects of substrate-induced strain, finite size and electron irradiation-induced defects have been studied on individual micron-sized domains of the organic charge transfer compound tetrathiafulvalene-tetracyanoquinodimethane (TTF-TCNQ) by temperature-dependent conductivity and current-voltage measurements. The individual domains have been isolated by focused ion beam etching and electrically contacted by focused ion and electron beam induced deposition of metallic contacts. The temperature-dependent conductivity follows a variable range hopping behavior which shows a crossover of the exponent as the Peierls transition is approached. The low temperature behavior is analyzed within the segmented rod model of Fogler, Teber and Shklowskii, as originally developed for a charge-ordered quasi one-dimensional electron crystal. The results are compared with data obtained on as-grown and electron irradiated epitaxial TTF-TCNQ thin films of the two-domain type
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