Relevant bibliographies by topics / Sequential deposition

Academic literature on the topic 'Sequential deposition'

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Published: 10 December 2022
Last updated: 28 January 2023

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Journal articles on the topic "Sequential deposition"

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Wang, X., J. Ma, A. Maximenko, E. A. Olevsky, M. B. Stern, and B. M. Guenin. "Sequential deposition of copper/alumina composites." Journal of Materials Science 40, no. 12 (June 2005): 3293–95. http://dx.doi.org/10.1007/s10853-005-2704-2.

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Wang, X., J. Ma, A. Maximenko, E. A. Olevsky, M. B. Stern, and B. M. Guenin. "Sequential deposition of copper/alumina composites." Journal of Materials Science 40, no. 18 (September 2005): 4963–65. http://dx.doi.org/10.1007/s10853-005-3869-4.

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Eisenberg, Eli, and Asher Baram. "Diffusional relaxation in random sequential deposition." Journal of Physics A: Mathematical and General 30, no. 9 (May 7, 1997): L271—L276. http://dx.doi.org/10.1088/0305-4470/30/9/003.

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Ermanova, Inga, Narges Yaghoobi Nia, Enrico Lamanna, Elisabetta Di Bartolomeo, Evgeny Kolesnikov, Lev Luchnikov, and Aldo Di Carlo. "Crystal Engineering Approach for Fabrication of Inverted Perovskite Solar Cell in Ambient Conditions." Energies 14, no. 6 (March 22, 2021): 1751. http://dx.doi.org/10.3390/en14061751.

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In this paper, we demonstrate the high potentialities of pristine single-cation and mixed cation/anion perovskite solar cells (PSC) fabricated by sequential method deposition in p-i-n planar architecture (ITO/NiOX/Perovskite/PCBM/BCP/Ag) in ambient conditions. We applied the crystal engineering approach for perovskite deposition to control the quality and crystallinity of the light-harvesting film. The formation of a full converted and uniform perovskite absorber layer from poriferous pre-film on a planar hole transporting layer (HTL) is one of the crucial factors for the fabrication of high-performance PSCs. We show that the in-air sequential deposited MAPbI3-based PSCs on planar nickel oxide (NiOX) permitted to obtain a Power Conversion Efficiency (PCE) exceeding 14% while the (FA,MA,Cs)Pb(I,Br)3-based PSC achieved 15.6%. In this paper we also compared the influence of transporting layers on the cell performance by testing material depositions quantity and thickness (for hole transporting layer), and conditions of deposition processes (for electron transporting layer). Moreover, we optimized second step of perovskite deposition by varying the dipping time of substrates into the MA(I,Br) solution. We have shown that the layer by layer deposition of the NiOx is the key point to improve the efficiency for inverted perovskite solar cell out of glove-box using sequential deposition method, increasing the relative efficiency of +26% with respect to reference cells.
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Kant, Pallav, Andrew L. Hazel, Mark Dowling, Alice B. Thompson, and Anne Juel. "Sequential deposition of microdroplets on patterned surfaces." Soft Matter 14, no. 43 (2018): 8709–16. http://dx.doi.org/10.1039/c8sm01373j.

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We use a combination of experiments and numerical modelling to investigate the influence of physico-chemical-patterned substrates on the spreading of fluid deposited as a partially overlapping sequence of droplets via inkjet printing. We find that both topography and wettability variations are required for robust pixel filling without overspill.
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NOVOTNY, M. A., and A. KOLAKOWSKA. "MIXING DIFFERENT RANDOM DEPOSITIONS IN NONEQUILIBRIUM SURFACE GROWTH MODELS." International Journal of Modern Physics C 20, no. 09 (September 2009): 1377–85. http://dx.doi.org/10.1142/s0129183109014448.

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An exact solution is presented for mixing two or more different types of Random Deposition (RD) nonequilibrium surface growth processes. The depositions may be made in a sequential mode, or in a random mode by first randomly choosing the lattice site for deposition. The results hold in all dimensions d. Simulations are presented in d = 1 for comparison. Furthermore, a mean-field type of approach to mixing RD with other surface growth processes is tested against the exact solution.
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Groenendijk, D. J., and S. Gariglio. "Sequential pulsed laser deposition of homoepitaxial SrTiO3thin films." Journal of Applied Physics 120, no. 22 (December 14, 2016): 225307. http://dx.doi.org/10.1063/1.4971865.

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Zhang, Lijian, Chunyan Wu, Weifeng Liu, Shangfeng Yang, Mingtai Wang, Tao Chen, and Changfei Zhu. "Sequential deposition route to efficient Sb2S3 solar cells." Journal of Materials Chemistry A 6, no. 43 (2018): 21320–26. http://dx.doi.org/10.1039/c8ta08296k.

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Penrose, Mathew D., and J. E. Yukich. "Limit Theory for Random Sequential Packing and Deposition." Annals of Applied Probability 12, no. 1 (February 2002): 272–301. http://dx.doi.org/10.1214/aoap/1015961164.

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Danwanichakul, Panu, and Eduardo D. Glandt. "Sub-monolayer growth by sequential deposition of particles." Journal of Colloid and Interface Science 294, no. 1 (February 2006): 38–46. http://dx.doi.org/10.1016/j.jcis.2005.07.010.

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Dissertations / Theses on the topic "Sequential deposition"

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Brun, Soren Erik. "Sequential scouring, alternating patterns of erosion and deposition, laboratory experiments and mathematical modelling." Thesis, National Library of Canada = Bibliothèque nationale du Canada, 1998. http://www.collectionscanada.ca/obj/s4/f2/dsk2/tape15/PQDD_0001/NQ35117.pdf.

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Sy, Piecco Kurt Waldo. "Chemically-Patterned Substrates via Sequential Photoinitiated Thiol-ene Reactions asTemplates for the Deposition of Molecules and Materials on Surfaces." Ohio University / OhioLINK, 2019. http://rave.ohiolink.edu/etdc/view?acc_num=ohiou1553174280949411.

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Abdullahi, Mohamed Farah. "Modification of glassy carbon electrode (GCE) with prussian blue as a mediator on carbon nanotube materials through sequential deposition." Thesis, Vaal University of Technology, 2012. http://hdl.handle.net/10352/387.

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Prussian blue (PB) nanoparticles were synthesized from FeCl3.6H2O, K4[Fe(CN)6].3H2O, and from Fe(NO3)3.9H2O and K4[Fe(CN)6].3H2O, and then characterized by Fourier transform infrared (FT-IR), Ultraviolet-visible spectroscopy, X-ray diffraction (XRD), Energy dispersive spectroscopy (EDS), Scanning electron microscopy (SEM), Raman spectroscopy and thermogravimetric analysis. Graphene oxide and carbon nanotubes were also synthesized and characterized. PB nanoparticles, carbon nanotubes (CNT), graphene oxide (GO) and cetyltrimethylammonium bromide (CTAB) were sequentially deposited onto glassy carbon electrode surface to form chemically modified electrode for the detection of hydrogen peroxide (H2O2) and dopamine. The following electrodes were fabricated, GC-PB, GC-MWCNT, GCGO, GC-CTAB, GC-MWCNT-PB, GC-GO-PB and GC-CTAB-PB. Cyclic and Square wave voltammetric techniques were used to measure the hydrogen peroxide detectability of the electrodes at pH ranges of (3 - 7.4) in 0.1M phosphate buffer solution, in the absence or presence of 25 μL of H2O2. The GC-CNT-PB, GC-GO-PB,GC-CTAB-PB electrodes showed a good response for the detection of hydrogen peroxide in both acidic and neutral media while the GCPB electrode only showed good response in acidic media.
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Aviziotis, Ioannis. "Chemical vapor deposition of Al, Fe and of the Al13Fe4 approximant intermetallic phase : experiments and multiscale simulations." Thesis, Toulouse, INPT, 2016. http://www.theses.fr/2016INPT0100/document.

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Des couches minces contenant des phases intermétalliques présent et des propriétés et de combinaisons de propriétés qui ne sont que partiellement explorées. Elles portent des solutions potentielles pour conférer des multifonctionnalités à des matériaux avancés requis par les secteurs industriels et sont source derupture et de l'innovation. Leur élaboration par dépôt chimique en phase vapeur à partir de précurseurs métallo-organiques (MOCVD) permet un dépôt conforme sur, et la fonctionnalisation de surfaces complexes, avec un temps de traitement court et à un coût modéré.Pour ceci, il est nécessaire de contrôler les réactions chimiques complexes et des mécanismes de transport impliqués. La modélisation informatique du procédé, alimentée avec des données obtenues par des expériences de dépôt ciblées, est un outil intégré pour l'étude et la compréhension des phénomènes qui se produisent à différentes échelles,de l’échelle macroscopique à celle nanométrique. La MOCVD de composés intermétalliques Al-Fe est étudiée en tant que paradigme de la mise en oeuvre d'une telle approche combinée, expérimentale et théorique. La phase approximanteAl13Fe4 est particulièrement ciblée,en raison de son intérêt comme alternative peu onéreuse aux catalyseurs à base de métaux noble dans l'industrie chimique. La mise au point du dépôt de la phase Al13Fe4est subordonnée à l'étude des proc /min à 185oC. La simulation du procédé prédit des vitesses de croissance en bon accord avec ces résultats, en particulier dans la gamme 139oC-227oC. La modélisation multi-échelle prédit la rugosité RMS avec précision, permettant ainsi le contrôle des propriétés telles que la résistivité électrique. La possibilité d'obtenir des films MOCVD de Fe à faible contamination en O et C est explorée dans la gamme 130oC-250oC à partir de fer pentacarbonyle, Fe(CO)5. La morphologie de la surface des films dépend fortement de la température de dépôt; elle devient plus lisse au-dessus de200oC, qui correspond aussi à la vitesse de croissance maximale, 60nm/min. La vitesse de dépôt diminue fortement lorsque la pression augmente. Les prédictions de la modélisation macroscopique reproduisent précisément ce comportement. Elles indiquent que la diminution de la vitesse de croissance à des températures et des pressions élevées est due à l’augmentation de la décomposition du précurseur en phase gazeuse et à l'inhibition de la réactivité de surface par le ligand CO. Le modèle multi échelle conduit à des valeurs RMS en bon accord avec les mesures expérimentales, en particulier à des températures plus élevées. Suite à l’étude des deux procédés, des co-dépôts d'Al-Fe effectués à 200oCrésultent en des films riches en Alavec une microstructure poreuse et rugueuse. Ceux-ci ne contiennent pas de phases intermétalliques et sont riches en oxygène dû à la réaction d'Al avec les ligandscarbonyles. Afin d’éliminer la contamination, des dépôts séquentiels d'Al et de Fe sont réalisés, ce dernier dans des conditions modifiées à 140oC, 40Torr et 10 min. Ces films sont exemptes d’hétéroélements et présentent un rapport atomique Al:Fe13:4. Diffraction des rayons X et microscopies électroniques révèlent qu’un recuit in situ à 575oC pendant 1 h conduit à des films à gradient de la composition sur l'épaisseur,composés de la phase approximantem-Al13Fe4 conjointement avec des phases intermétalliques Al-Fesecondaires. Il est ainsi démontré que des procédés MOCVD sont appropriés pour obtenir des films constitués d'alliages intermétalliques.Ces films multifonctionnels,appliqués de façon conforme sur des surfaces complexes sont utiles pour un grand nombre d'applications
Films containing intermetallic compounds exhibit properties and combination of properties which are only partially explored. They carry potential solutions to confer multifunctionality to advanced materials required by industrial sectors and to become a source of breakthrough and innovation.Metalorganic chemical vapor deposition (MOCVD) potentially allows conformal deposition on, and functionalization of complex surfaces, with high throughput and moderate cost. For this reason, it is necessary to control the complex chemical reactions and the transport mechanisms involved in a MOCVD process. In this perspective, computational modeling of the process, fed with experimental information from targeted deposition experiments, provides an integrated tool for the investigation and the understanding of the phenomena occurring at different length scales, from the macro- to the nanoscale. The MOCVD of Al-Fe intermetallic compounds is investigated in the present thesis as a paradigm of implementation of such a combined, experimental and theoretical approach. Processing of the approximant phase Al13Fe4 is particularly targeted, due to its potential interest as low-cost and environmentally benign alternative to noble metal catalysts in the chemical industry. The attainment of the targeted Al13Fe4 intermetallic phase passes through the investigation of the MOCVD of unary Al and Fe films. The MOCVD of Al from dimethylethylamine alane (DMEAA) in the range 139oC-241oC results in pure films. Increase of the deposition temperature yields higher film density and decreased roughness. The Aldeposition rate increases to a maximum of 15.5 nm/min at 185oC and then decreases. Macroscopic simulations of the process predictdeposition rates in sufficient agreement with experimental measurements, especially in the range 139oC-227oC. At higher temperatures, competitive gas phase and surface phenomena cannot be captured by the applied model. Multiscale modeling of the process predicts the RMS roughness of the films accurately, thus allowing the control of properties such as electrical resistivity which depend on the microstructure. The MOCVD of Fe from iron pentacarbonyl, Fe(CO)5, is investigated in the range 130oC-250oC for the possibility toobtain fairly pure Fe films with low Oand C contamination. The surface morphology depends strongly on the temperature and changes are observed above 200oC. The Fe deposition rate increases up to 200oC, to a maximum of 60 nm/min, and then decreases. Moreover, the deposition rate decreases sharply with increasing pressure. Computational predictions capture accurately the experimental behavior and they reveal that the decrease athigher temperatures and pressures is attributed to the high gas phase decomposition rate of the precursor and to inhibition of the surface fromCO. The multiscale model calculates RMS roughness in good agreement with experimental data, especially at higher temperatures. Upon investigation of the two processes, aseries of Al-Fe co-depositions performed at 200oC results in Al-rich films with a loose microstructure. They contain no intermetallic phases and they are O-contaminated due to the reaction of the Al with the carbonyl ligands. Sequential deposition of Al and Fe followed by in situ annealing at 575oC for 1 h is applied to bypass the Ocontamination. The process conditions of Fe are modified to 140oC, 40 Torr and 10 min resulting in O-free films with Al:Fe atomic ratio close to the targeted 13:4 one. Characterization techniques including X-ray diffraction, TEM and
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Mangan, Carmel Mary. "The sequestration of phosphate by iron phases in the sediments from Lake Rotorua, New Zealand." The University of Waikato, 2007. http://hdl.handle.net/10289/2238.

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A sequential extraction method was used to determine which dominant sedimentary mineral phase was involved in phosphorus retention in the sediments of Lake Rotorua and to verify the importance of iron phases in the role as a phosphorus sink. The observed influence of the experimental conditions upon the extent of phosphate adsorption to various iron phases shows a considerable quantity of phosphorus is present in the reducible phase and in the residual mineral phase. The phosphorus associated with iron(III) oxide phases was released into solution under reducing conditions when ferric iron oxide/oxyhydroxides, including amorphous and poorly crystalline Fe(III) phases, were solubilized. The residual primary and secondary mineral phases remained stable in the sediments until they were exposed to extremely acidic media analogous to strongly reducing conditions. Manganese is not involved in phosphorus retention to the same extent as iron. Aluminium phases present were released from surface complexes with relative ease and also from mineral structures under the prevailing conditions. The results show a strong agreement between aluminium and phosphorus suggesting it is associated with various aluminium phases to some extent. The sediments of Lake Rotorua are rich in organic-bound P which is released when organic material is oxidized under conditions analogous to anaerobic degradation. The degradation of refractory organic material represents a significant source of phosphorus for incorporation into diagenetic minerals forming in oxic and anoxic layers of the sediment. Heavy liquid separation of the sediments concentrated the small quantities of dense minerals into a separate fraction and the presence of iron sulfides could be verified. Three density fractions obtained by this method separated the diatoms (d less than 2.6 g cm-3), the silicates (d greater than 2.6 less than 3.7 g cm-3) and the heavy minerals (d greater than 3.7 g cm-3) present in the sediment sample. In the heavy mineral phase spherulitic framboidal pyrite and rhombohedrial siderite were observed by scanning electron microscopy (SEM). Energy dispersive x-ray fluorescence (XRF) analysis of the framboidal pyrite detected significant fluorescence's for sulphur and iron. The elemental analysis of siderite characterised it as an iron-rich, non-sulfidic particle with no phosphorus fluorescence. Particles were also observed that had a variable morphology to the framboidal pyrite minerals but similar ratio of Fe to S in the XRF spectrum. It is likely they are other stable forms of iron sulfides or pyrites in various stages of diagenetic dissolution. Digestion of the three density fractions shows the heavy mineral phase is significantly enriched in sulfur and in iron confirming the presence of sulfides. The sulfide-forming trace metals are concentrating in the heavy mineral phase but a progressive enrichment of trace metals down core is not found in the results. Many of the trace elements show maximum concentrations in the Tarawera tephra. There is a good agreement between iron and phosphorus in both treatments that implies iron phases are the predominant phosphorus fixers in the sediments of Lake Rotorua. However the identity of the phosphorus sink could not be confirmed by SEM or XRF analysis of the heavy minerals. The most likely explanations for the observed concentrations of iron and phosphorus and enrichment in the heavy mineral fraction are the persistence of the highly insoluble crystalline iron oxyhydroxides (goethite) in reducing sediments or the formation of the reduced iron mineral vivianite. Considering the density of vivianite it would have being taken into the heavy fraction by default which would account for the enrichment demonstrated by the solution analysis.
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Silva, Camilla Zacché da. "Metodologias de inserção de dados sob mecanismo de falta mnar para modelagem de teores em depósitos multivariados heterotópicos." reponame:Biblioteca Digital de Teses e Dissertações da UFRGS, 2018. http://hdl.handle.net/10183/178441.

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Ao modelar-se depósitos minerais é comum enfrentarmos o problema de estimar múltiplos atributos possivelmente correlacionados, onde algumas variáveis são amostradas menos densamente do que outras. A falta de dados impõe um problema que requer atenção antes de qualquer modelagem subsequente. Precisamos, ao final, de modelos que sejam estatisticamente representativos. A maioria dos conjuntos de dados de problemas práticos são amostrados de maneira heterotópica e, para obter resultados coerentes, é preciso entender os motivos pelos quais alguns dados faltam e quais são os mecanismos que influenciaram a ausência de informações. A teoria de dados faltantes relaciona as amostras ausentes com aquelas medidas através de três mecanismos distintos: Faltante Completamente Aleatório (Missing Completely At Random - MCAR), Faltante Aleatório (Missing At Random - MAR) e Faltante Não Aleatório (Missing Not At Random - MNAR). O último mecanismo é extremamente complexo e a literatura recomenda ser tratado inicialmente como um mecanismo MAR. E após uma transformação fixa deve ser aplicada aos valores complementados para que estes se transformem em valores MNAR Embora existam métodos estatísticos clássicos para lidar com dados faltantes, tais abordagens ignoram a correlação espacial, uma característica que ocorre naturalmente em dados geológicos. A metodologia adequada para tratar com a falta de dados geológicos é a atualização bayesiana, em que se inserem valores sob mecanismo MAR considerando a correlação espacial. No presente estudo, a atualização bayesiana foi combinada com transformações fixas para tratar o mecanismo de falta de dados MNAR em dados geológicos. A transformação fixa aqui empregada é baseada no erro de inserção gerado em um cenário MAR no conjunto de dados. Assim, com o conjunto completo resultante foi utilizado em uma simulação sequencial gaussiana dos teores de uma base de dados multivariada, apresentando resultados satisfatórios, superiores aos obtidos por meio da cossimulação sequencial gaussiana, não inserindo qualquer viés no modelo final.
When modeling mineral deposits, it is common to face the problem of estimating multiple attributes possibly correlated where some variables are more densely sampled then others. Missing data imposes a problem that requires attention prior to any subsequent modeling. The later requires estimation models statistically representative. Most practical data sets are often heterotopically sampled, and to obtain coherent results one must understand the reasons why there are missing data and what are the mechanisms that cause the absence of information. The theory of missing data relates the missing samples to those measured through three different mechanisms: Missing Completely At Random (MCAR), Missing At Random (MAR), and Missing Not At Random (MNAR). The last mechanism is quite complex to deal with, and the literature recommends being treated as a MAR mechanism and after a fixed transform should be applied to the imputed values so that these turn into MNAR imputed values. Even though there are classical statistical methods to deal with missing data, such approaches ignore spatial correlation, a feature that occurs naturally in geological data. The adequate methodology to deal with missing geologic data is Bayesian Updating, which approaches the MAR mechanism and accounts for spatial correlation. In the present study, bayesian updating was used combined with fixed transforms to treat MNAR missing data mechanism in geologic data. The fixed transform herein used is based on the error of MAR imputation on the data set. The resulting complete set was then used on a sequential gaussian simulation of the grades on a multivariate data set, presenting satisfactory results, superior to those obtained through sequential gaussian cossimulation, not inserting any biases on the final model.
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Kao, Shu-Chen, and 高書辰. "The sequential deposition of MAPbI3 on TiO2 nanorod-based perovskite solar cell." Thesis, 2019. http://ndltd.ncl.edu.tw/cgi-bin/gs32/gsweb.cgi/login?o=dnclcdr&s=id=%22107NCHU5693009%22.&searchmode=basic.

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碩士
國立中興大學
精密工程學系所
107
Hybrid organic-inorganic perovskite is the most promising solar cell material in recent years. In this thesis, the rutile phase of titanium dioxide with the nanorod structure is synthesized by the hydrothermal method. The influences of the microstructure of titanium dioxide on sequential deposited perovskites and their conversion efficiency are systemically investigated. This thesis can be basically divided into two parts. The first part of the thesis is mainly focused on the study of the reaction temperature, the reaction concentration and the reaction time during the hydrothermal synthesis. The scanning electron microscope (SEM) and X-ray diffractometer (XRD) were used to analyze the microstructure, surface morphology and crystalline structure of the as-synthesized titanium dioxide and understand the relationship between their properties and the hydrothermal processing parameters. The second part of the thesis is mainly focused on the effect of nanorod titanium dioxide with different lengths on the sequential deposited perovskites. In the experiment, the methylammonium lead iodide (CH3NH3PbI3) was selected and prepared by the sequential deposition on a series of nanorod titanium dioxides with different lengths and commonly used mesoporous titanium dioxide. The analyses of the microstructure, the crystallinity, the optical property of as-prepared perovskites were performed to investigate the relationship between the sequential deposited perovskites and different titanium dioxides. Our experimental result shows that the perovskite solar cell using nanorod titanium dioxide can exhibit a conversion efficiency of 13% because of the better transition of lead iodide to perovskite and the improved carrier collection.
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"Development of a Co–deposition method for Deposition of Low–Contamination Pyrite Thin Films." Master's thesis, 2016. http://hdl.handle.net/2286/R.I.38609.

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abstract: Pyrite is a 0.95 eV bandgap semiconductor which is purported to have great potential in widespread, low–cost photovoltaic cells. A thorough material selection process was used in the design of a pyrite sequential vapor deposition chamber aimed at reducing and possibly eliminating contamination during thin film growth. The design process focused on identifying materials that do not produce volatile components when exposed to high temperatures and high sulfur pressures. Once the materials were identified and design was completed, the ultra–high vacuum growth system was constructed and tested. Pyrite thin films were deposited using the upgraded sequential vapor deposition chamber by varying the substrate temperature from 250°C to 420°C during deposition, keeping sulfur pressure constant at 1 Torr. Secondary Ion Mass Spectrometry (SIMS) results showed that all contaminants in the films were reduced in concentration by orders of magnitude from those grown with the previous system. Characterization techniques of Rutherford Back–scattering Spectrometry (RBS), X–Ray Diffraction (XRD), Raman Spectroscopy, Optical Profilometry and UV/Vis/Near–IR Spectroscopy were performed on the deposited thin films. The results indicate that stoichiometric ratio of S:Fe, structural–quality (epitaxy), optical roughness and percentage of pyrite in the deposited thin films improve with increase in deposition temperature. A Tauc plot of the optical measurements indicates that the pyrite thin films have a bandgap of 0.94 eV.
Dissertation/Thesis
Masters Thesis Materials Science and Engineering 2016
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Wang, Jian-Hua, and 王建驊. "The study of solvent evaporation on sequential deposition process for perovskite solar cells." Thesis, 2018. http://ndltd.ncl.edu.tw/handle/t2m396.

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碩士
國立中興大學
精密工程學系所
106
The organic-inorganic perovskite solar cell (PSCs) is considered one of the most promising candidates for the next generation photovoltaic device because of its fast progress of the conversion efficiency over 20%. However, the behavior of evaporated solvents (DMSO, DMF, IPA and so forth) during the perovskite film formation can be strongly correlated with the quality of the resulting perovskite film, playing a crucial role in repeatedly obtaining the good device performance. Accordingly, the homemade facility is developed for controlling the solvent evaporation during the sequential CH3NH3PbI3 perovskite deposition. Our work in this thesis can be mainly divided into three parts. In the first part, the basic study of sequential perovskite film growth is conducted through different process parameters in order to obtain the optimized film quality. In the second part, the as-coated PbI2 is treated with vacuum-assisted process (VAP) by our developed facility. Our result shows that the PbI2 film quality can be tuned by using the different time and pressure during the VAP, and thereby affect the perovskite morphology. The different ratio of DMSO to DMF is also used in order to understand the solvent effect. In the third part, the VAP is applied to as-coated CH3NH3I in order to further understand the role of VAP played during the sequential perovskite deposition process.
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Rizwan, Tania. "Colloidal particle deposition onto charge-heterogeneous substrates." Phd thesis, 2009. http://hdl.handle.net/10048/743.

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Thesis (Ph. D.)--University of Alberta, 2009.
Title from PDF file main screen (viewed on Nov. 27, 2009). "A thesis submitted to the Faculty of Graduate Studies and Research in partial fulfillment of the requirements for the degree of Doctor of Philosophy, Department of Mechanical Engineering, University of Alberta." Includes bibliographical references.
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Books on the topic "Sequential deposition"

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Brun, Søreb Erik. Sequential scouring: Alternating patterns of erosion and deposition-laboratory experiments and mathematical modelling. 1998.

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Book chapters on the topic "Sequential deposition"

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Yamamoto, Kiyoshi, Koh-ichi Kubo, Nobuyuki Sugii, Michiharu Ichikawa, and H. Yamauchi. "Sequential Deposition and Characterization of M1−xCuO2±δ." In Advances in Superconductivity V, 235–38. Tokyo: Springer Japan, 1993. http://dx.doi.org/10.1007/978-4-431-68305-6_50.

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Nakazawa, Takahiro, Toshimasa Suzuki, and Haruo Hirose. "Electrochemical Growth of Bi-Sr-Ca-Cu-O Films on Ag Substrates by Sequential Deposition." In Advances in Superconductivity V, 1017–20. Tokyo: Springer Japan, 1993. http://dx.doi.org/10.1007/978-4-431-68305-6_228.

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Kamei, M., I. Yoshida, K. Suzuki, T. Morishita, and S. Tanaka. "Growth Characteristics of Bi-Sr-(Ca)-Cu-O Films Prepared by ECR Plasma Assisted Sequential Deposition." In Advances in Superconductivity III, 1077–80. Tokyo: Springer Japan, 1991. http://dx.doi.org/10.1007/978-4-431-68141-0_244.

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Takahashi, H., N. Homma, S. Kawamoto, H. Kondo, K. Suzuki, and T. Morishita. "In-situ Preparation of Superconducting Y-Ba-Cu-O Films by Sequential Deposition Using 40MHz Magnetron Sputtering." In Advances in Superconductivity II, 793–96. Tokyo: Springer Japan, 1990. http://dx.doi.org/10.1007/978-4-431-68117-5_169.

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Kazda, M., and G. Glatzel. "Dry Deposition, Retention and Wash-Off Processes of Heavy Metals in Beech Crowns: Analysis of Sequentially Sampled Stemflow." In Atmospheric Pollutants in Forest Areas, 215–22. Dordrecht: Springer Netherlands, 1986. http://dx.doi.org/10.1007/978-94-009-4736-8_18.

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"Structure and Properties of Bi2Sr2Can_1Cun02n+4 Films Prepared by Sequential Sputter Deposition." In Bismuth-Based High-Temperature Superconductors, 565–96. CRC Press, 1996. http://dx.doi.org/10.1201/9781482273472-29.

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Liu, Ying-Chi, Wen-Hsiung Lin, Wen-Hui Wang, and Hsin-Fu Chang. "Autothermal reaction of ethanol through Pd-Ag membrane reactor prepared by sequential electroless deposition." In New Developments and Application in Chemical Reaction Engineering, 817–20. Elsevier, 2006. http://dx.doi.org/10.1016/s0167-2991(06)81722-2.

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"Whirling Disease: Reviews and Current Topics." In Whirling Disease: Reviews and Current Topics, edited by ELIZABETH MACCONNELL and E. RICHARD VINCENT. American Fisheries Society, 2002. http://dx.doi.org/10.47886/9781888569377.ch9.

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<EM>ABSTRACT. </EM>Whirling disease is a chronic inflammatory disease in salmonid fish caused by the myxosporean parasite <em>Myxobolus cerebralis</em>. The disease, first recognized in cultured rainbow trout <em>Oncorhynchus mykiss</em>, is characterized by the radical tail-chasing behavior of infected fish. The parasite is enzootic in free ranging and cultured populations of trout in areas of salmonid aquaculture, except South America. Recent reports of severe population declines among wild trout associated with whirling disease has caused great concern and renewed interest in this pathogen. The parasite has a sequential affinity for the skin, nerves, and, finally, skeletal cartilage, in the fish host. Abundant cartilage in the skeleton of young trout renders them extremely susceptible to the effects of the disease. Most salmonid species are susceptible to infection with <em>M. cerebralis</em>, but susceptibility varies among species and may also vary among strains and individual fish within a population or a similarly exposed group. Rainbow trout and anadromous steelhead are highly susceptible to whirling disease. The severity of the disease and mortality are related to age of the fish, when first exposed, and parasite dose. Trophozoite stages of the parasite lyse cartilage, cause an inflammatory response, and may interfere with normal bone deposition in the salmonid host. In severely infected fish, growth rates are depressed during active infection, and behavioral effects and severe skeletal deformities compromise functions such as swimming and feeding. The effects of <em>M. cerebralis </em>on the salmonid host are determined by factors such as species, age, size, parasite dose, immune response, and water temperature. Understanding the interaction of these factors in waters where <em>M. cerebralis </em>is present is critical to the future management of healthy wild trout populations.
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Conference papers on the topic "Sequential deposition"

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Ghafouri-Azar, R., S. Shakeri, S. Chandra, and J. Mostaghimi. "Numerical Simulation of Offset Deposition for Sequential Tin Droplets." In ITSC2002, edited by C. C. Berndt and E. Lugscheider. Verlag für Schweißen und verwandte Verfahren DVS-Verlag GmbH, 2002. http://dx.doi.org/10.31399/asm.cp.itsc2002p0972.

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Abstract The spreading and solidification of a molten droplet is governed a number of factors such as fluid inertia, viscosity, surface tension, surface wettability, heat transfer between the droplet and substrate, and surface thermal properties. Most numerical and experimental studies of droplet impact have considered a single molten droplet landing on a flat, solid surface. This paper investigates the sequential deposition of tin droplets with their centers offset using a three-dimensional model of droplet impact and solidification. In this study, the successive deposition of two tin droplets on a stainless steel substrate is simulated and the results are compared with photographs of impacting droplets. Paper includes a German-language abstract.
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Dhare, Vaishali, and Usha Mehta. "Single missing cell deposition defect analysis of sequential reversible circuit." In 2017 Nirma University International Conference on Engineering (NUiCONE). IEEE, 2017. http://dx.doi.org/10.1109/nuicone.2017.8325621.

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Akkoyunlu, O. "A STUDY OF WET DEPOSITION FLUX USING THE SEQUENTIAL SAMPLING TECHNIQUE." In SGEM2011 11th International Multidisciplinary Scientific GeoConference and EXPO. Stef92 Technology, 2011. http://dx.doi.org/10.5593/sgem2011/s17.102.

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Reyes-Vallejo, Odin, Rocio M. Sanchez-Albores, Arturo Fernandez-Madrigal, Francisco J. Cano, C. A. Meza-Avendano, J. J. Diaz, A. Ashok, and P. J. Sebastian. "Chemical Bath Deposition of Cu2O Thin Films on FTO Substrates: Effect of Sequential Deposition." In 2022 19th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE). IEEE, 2022. http://dx.doi.org/10.1109/cce56709.2022.9975937.

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Sahli, Florent, Jeremie Werner, Brett A. Kamino, Matthias Brauninger, Terry Chien-Jen Yang, Peter Fiala, Gizem Nogay, et al. "Hybrid sequential deposition process for fully textured perovskite/silicon tandem solar cells." In 2018 IEEE 7th World Conference on Photovoltaic Energy Conversion (WCPEC) (A Joint Conference of 45th IEEE PVSC, 28th PVSEC & 34th EU PVSEC). IEEE, 2018. http://dx.doi.org/10.1109/pvsc.2018.8547435.

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Kobrin, B., J. Chin, and W. R. Ashurst. "Vapor Deposition of Composite Organic-Inorganic Films." In World Tribology Congress III. ASMEDC, 2005. http://dx.doi.org/10.1115/wtc2005-64335.

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Results on the thermal and immersion stability of ultra-thin composite films created by a deposition method call MVD™ (Molecular Vapor Deposition [1]) are reported. It is observed that these composite films were denser and more stable in thermal and immersion applications when compared to traditional self-assembled monolayer (SAM) films. These improved films were created by a special “sequential” or “layered” deposition process sequence. The MVD™ composite coatings can be deposited at room temperature on a variety of materials such as polymers, fibers, metals, alloys and other materials which normally do not allow films to form with complete surface coverage.
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Zhang, N., Z. Charlie Zheng, L. Glasgow, and B. Braley. "Particle Deposition in a Room-Scale Chamber With Particle Injection." In ASME 2005 Fluids Engineering Division Summer Meeting. ASMEDC, 2005. http://dx.doi.org/10.1115/fedsm2005-77090.

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A model simulating the deposition of small particles with turbulent transport, sedimentation, and coagulation, is presented. Experimental measurements were conducted in a room-scale chamber using a specially designed sequential sampler. The measured deposition-rate data are compared with the simulation results. Distributions of particle-number density at different times are plotted in several viewing planes to facilitate discussion of the particle distribution patterns.
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Shui Hsiang Su, M. Yokoyama, and Yan Kuin Su. "A 10-in. Diagonal ZNS:MN Tfel Panel Fabricated By A Sequential Vacuum Deposition Apparatus." In 1997 Asian Symposium on Information Display. IEEE, 1997. http://dx.doi.org/10.1109/asid.1997.631404.

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Kim, Jae-Hyung, and Akihiro Sasoh. "Drag Reduction Performance due to Repetitive Laser Pulses on the Blunt Body." In ASME-JSME-KSME 2011 Joint Fluids Engineering Conference. ASMEDC, 2011. http://dx.doi.org/10.1115/ajk2011-15002.

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Supersonic wave drag reduction due to the repetitive laser induced energy deposition is performed experimentally in this study. Laser pulses are irradiated through a convex lens installed in side of the in-draft wind tunnel of Mach 1.94. The maximum frequency and power of the energy deposition is limited up to 50kHz and 400W. In order to estimate the drag reduction, time-averaged drag force is measured by a force balance system and stagnation pressure history is synchronized with corresponding sequential schlieren images captured by high-speed camera. Drag reduction performance is linearly increased up to 21% with input laser power. The power gain which only depends on the pulse energy, is realized by approximately 7. Virtual spike formation induced by highrepetitive energy depositions is remarkably discussed in the visualization results.
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Zhu, Rui. "Mesoporous PbI2 Scaffold for High-Performance Planar Heterojunction Perovskite Solar Cells via Sequential Deposition Process." In Photonics for Energy. Washington, D.C.: OSA, 2015. http://dx.doi.org/10.1364/pfe.2015.pt4a.3.

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Reports on the topic "Sequential deposition"

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Huckaby, Dale A., and L. Blum. A Model for Sequential First Order Phage Transitions Occurring in the Underpotential Deposition of Metals,. Fort Belvoir, VA: Defense Technical Information Center, April 1991. http://dx.doi.org/10.21236/ada235623.

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