Dissertations / Theses on the topic 'Pulsed electro deposition'
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Alshekhli, Omar. "PULSED ELECTRON DEPOSITION AND CHARACTERIZATION OF NANOCRYSTALLINE DIAMOND THIN FILMS." Thesis, Laurentian University of Sudbury, 2013. https://zone.biblio.laurentian.ca/dspace/handle/10219/2078.
Full textHyde, Robert H. "Hollow-electrode pulsed plasma deposition of titanium and carbon thin films." [Tampa, Fla] : University of South Florida, 2006. http://purl.fcla.edu/usf/dc/et/SFE0001856.
Full textJenderka, Marcus. "Pulsed Laser Deposition of Iridate and YBiO3 Thin Films." Doctoral thesis, Universitätsbibliothek Leipzig, 2017. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-219334.
Full textThe present thesis reports on the thin film growth of ternary oxides Na2IrO3, Li2IrO3, Y2Ir2O7 and YBiO3. All of these oxides are candidate materials for the so-called topological insulator and spin liquid, respectively. These states of matter promise future application in quantum computation, and in magnetic memory and low-power electronic devices. The realization of the thin films presented here, thus represents a first step towards these future device applications. All thin films are prepared by means of pulsed laser deposition on various single-crystalline substrates. Their structural, optical and electronic properties are investigated with established experimental methods such as X-ray diffraction, spectroscopic ellipsometry and resistivity measurements. The structural properties of Na2IrO3 thin films, that were previously realized in the author’s M. Sc. thesis for the first time, are improved significantly by deposition of an intermediate ZnO layer. Single-crystalline Li2IrO3 thin films are grown for the first time and exhibit a defined crystal orientation. Measurement of the dielectric function gives insight into electronic excitations that compare well with single crystal samples and related iridates. From the data, an optical energy gap of about 300 meV is obtained. For Y2Ir2O7 thin films, a possible (111) out-of-plane preferential crystal orientation is obtained. Compared to chemical solution deposition, the pulsed laser-deposited YBiO3 thin films presented here exhibit a biaxial in-plane crystal orientation up to a significantly larger film thickness. From the measured dielectric function, a direct and indirect band gap energy is determined. Their magnitude provides necessary experimental feedback for theoretical calculations of the electronic structure of YBiO3, which are used in the prediction of the novel states of matter mentioned above. After the introduction and motivation of this thesis, the second chapter reviews the current state of the science of the studied thin film materials. The following two chapters introduce the sample preparation and the employed experimental methods, respectively. Subsequently, the experimental results of this thesis are discussed for each material individually. The thesis concludes with a summary and an outlook
Waller, Gordon Henry. "Template Directed Growth of Nb doped SrTiO3 using Pulsed Laser Deposition." Thesis, Virginia Tech, 2011. http://hdl.handle.net/10919/32723.
Full textMaster of Science
Nsengiyumva, Schadrack. "Formation and characterization of pulsed laser ablated magnetoresistive material." Thesis, Stellenbosch : Stellenbosch University, 2002. http://hdl.handle.net/10019.1/52852.
Full textENGLISH ABSTRACT: In this investigation the formation of thin film manganites and their electrical characteristics is studied. In order to see the effect of oxidation states on magneto-resistivity, 80% of Mn is replaced by Fe. Pulsed laser deposition (3 J/cm2), carried out in oxygen partial pressures ranging from 0.01 mbar to 1.00 mbar was used to fabricate the thin films from two target compositions, namely La2CaMn2.94Feo.0609 and La2CaMno.6Fe2.409. Films were deposited on Si< 100 >, MgO< 100 >, SrTi03< 100 > and LaAl03< 100 > single crystal substrates. Samples were characterized by RBS, AFM, SEM, and XRD. Electrical measurements were also carried out. One of the main characterization techniques in this investigation is Rutherford Backscattering Spectrometry (RBS). It has been shown that RBS is a very powerful characterization technique when used in conjunction with the RUMP simulation program. The effect of various parameters can be determined beforehand by RUMP simulation of the thin film structures to be investigated. Simulation shows that RBS is an excellent characterization tool for determining film thickness and stoichiometry. The role of oxygen uptake in La2CaMn3_xFexOg was investigated as the oxidation states of elements in manganite materials have a large effect on their magnetoresistive properties. The height of the La signal can be used as a measure of the oxygen content. RBS spectra of films deposited on single crystal silicon substrates at different ambient pressures show that the fit between simulated and measured RBS spectra improves with higher oxygen pressures, thereby indicating better quality manganite material. The RBS spectra also show that the films have good stoichiometry. Atomic force microscopy was used to determine the roughness of the thin films. The annealed film (average roughness 4.5 nm) shows a surface smoother than the non-annealed film (average roughness 5.3 nm). SEM measurements show that in the case of samples having a high Fe content, the crystallite size varies between about 0.04 11m and 0.10 11m, while for samples with high manganese content, the crystallinity varies between 0.03 jJ,m and 0.06jLm. Manganites were analyzed using Bragg-Brentano (28) X-ray diffraction. Measurements show that manganite films cannot be grown epitaxially on Si< 100 > and MgO< 100 > single crystals due to a large lattice mismatch. In the case of SrTi03 and LaAl03 several reflections and sharp peaks from the film can be seen, indicating reasonable epitaxial growth. SEM measurements of the samples however show polycrystallinity. Complete epitaxy has thus not occurred, but many grains have an epitaxial orientation. Resistance versus temperature (the room temperature to about 100 K) in zero magnetic field was measured for a La2CaMno.06Fe2.409 thin film and maximum resistance corresponding to about 108 K was found. At higher temperatures the resistance decreases as temperature increases. The manganite thin film therefore shows semiconductor behaviour. Resistance measurements carried out at different magnetic fields (0 - 1 T) show a small positive magnetoresistance of 0.83 %. Usually the magnetoresistance phenomenon is measured at higher magnetic fields and this could be the reason for our low value as well as the fact that the iron content could be too high.
AFRIKAANSE OPSOMMING: In hierdie ondersoek is die formasie en karakterisering van dunlagie manganiete ondersoek. Om die effek van oksidasie-toestand op magnetoresistiwiteit te bepaal, is 80% van die Mn verplaas deur Fe. Pulseerde laser deposissie(3 J/cm2), is uitgevoer by 'n parsiële suurstof druk tussen 0.10 en 1.00 mbar deur gebruik te maak van La2Ca Mn2.94Feo.o609 en La2CaMno.6Fe2.409 teiken skywe. Dunlagies was gedeponeer op Si
Zhang, Hong Bo. "Optical and electrical properties of ZnO thin films prepared by pulsed laser deposition." HKBU Institutional Repository, 2000. http://repository.hkbu.edu.hk/etd_ra/225.
Full textBowers, Cynthia Thomason. "Transmission Electron Microscopy Analysis of Silicon-Doped Beta-Gallium Oxide Films Grown by Pulsed Laser Deposition." Wright State University / OhioLINK, 2019. http://rave.ohiolink.edu/etdc/view?acc_num=wright1580120635333744.
Full textIbrahim, Noor Baa'yah. "Properties of yttrium iron garnet thin films grown by pulsed laser ablation deposition." Thesis, University of Warwick, 1999. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.343112.
Full textWei, Haoming, Jose Luis Barzola-Quiquia, Chang Yang, Christian Patzig, Thomas Höche, Pablo Esquinazi, Marius Grundmann, and Michael Lorenz. "Charge transfer-induced magnetic exchange bias and electron localization in (111)- and (001)-oriented LaNiO3/LaMnO3 superlattices." American Institute of Physics, 2017. https://ul.qucosa.de/id/qucosa%3A23554.
Full textSouri, Maryam. "ELECTRONIC AND OPTICAL PROPERTIES OF METASTABLE EPITAXIAL THIN FILMS OF LAYERED IRIDATES." UKnowledge, 2018. https://uknowledge.uky.edu/physastron_etds/60.
Full textGhaffari, Nastaran. "Electrochemical deposition of Graphene Oxide- metal nano-composite on Pencil-Graphite Electrode for the high sensitivity detection of Bisphenol A by Adsorptive Stripping Differential Pulse Voltammetry." University of the Western Cape, 2018. http://hdl.handle.net/11394/6336.
Full textElectrochemical platforms were developed based on pencil graphite electrodes (PGEs) modified electrochemically with reduced graphene oxide metal nanoparticles (ERGO–metalNPs) composite and used for the high-sensitivity determination of Bisphenol A (BPA) in water samples. Synergistic effects of both reduced Graphene Oxide sheets and metal nanoparticles on the performance of the pencil graphite electrode (PGE) were demonstrated in the oxidation of BPA by differential pulse voltammetry (DPV). A solution of graphene oxide (GO) 1 mg mL-1 and 15 ppm of metal stock solutions (1,000 mg L-1, atomic absorption standard solution) (Antimony or Gold) was prepared and after sonication deposited onto pencil graphite electrodes by cyclic voltammetry reduction. Different characterization techniques such as FT-IR, HR-SEM, XRD and Raman spectroscopy were used to characterize the GO and ERGO–metalNPs. Parameters that influence the electroanalytical response of the ERGO–SbNPs and ERGO–AuNPs such as, pH, deposition time, deposition potential, purging time were investigated and optimized. Well-defined, reproducible peaks with detection limits of 0.0125 μM and 0.062 μM were obtained for BPA using ERGO–SbNPs and ERGO–AuNPs respectively. The rGO-metalNPs–PGE was used for the quantification of BPA in tap water sample and proved to be suitable for the detection of BPA below USEPA prescribed drinking water standards of 0.087 μM.
Klemm, Robert. "Zyklische Plastizität von mikro- und submikrokristallinem Nickel." Doctoral thesis, Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2004. http://nbn-resolving.de/urn:nbn:de:swb:14-1085403884093-17423.
Full textKlemm, Robert. "Zyklische Plastizität von mikro- und submikrokristallinem Nickel." Doctoral thesis, Technische Universität Dresden, 2003. https://tud.qucosa.de/id/qucosa%3A23831.
Full textAkrobetu, Richard K. "The Interplay of Surface Adsorbates and Cationic Intermixing in the 2D Electron Gas Properties of LAO-STO Heterointerfaces." Case Western Reserve University School of Graduate Studies / OhioLINK, 2017. http://rave.ohiolink.edu/etdc/view?acc_num=case1491575404930072.
Full textKottman, Michael Andrew. "Additive Manufacturing of Maraging 250 Steels for the Rejuvenation and Repurposing of Die Casting Tooling." Case Western Reserve University School of Graduate Studies / OhioLINK, 2015. http://rave.ohiolink.edu/etdc/view?acc_num=case1416854466.
Full textLu, Chi-Yuan, and 盧啟原. "Investigation of Electro-Optical Semiconductor GaSe on Different Substrates by Pulsed Laser Deposition." Thesis, 2003. http://ndltd.ncl.edu.tw/handle/77303292707226405197.
Full text國立交通大學
光電工程所
91
We have successfully fabricated GaSe thin films on different substrates. From (004) peak position and FWHM of XRD, we observe that quality of GaSe/Si(111) series is the best compared to GaSe/GaN and GaSe/Sapphire at the same thickness due to small lattice mismatch. We also find that c-axis length of GaSe thin films were stretched larger at initial stage of deposition and the increasing amount (c) are GaSe/Sapphire, GaSe/GaN and GaSe/Si(111) in order. The crystalline of GaSe thin films can also be evaluated by Raman Al’ mode which vibrates along c-axis and E’(LO) mode which vibrates perpendicular to the c-axis of GaSe. From the analysis of FWHM of A1’mode, the tendency is identical compared with XRD result. In addition, we also find that the A1’mode shift to lower frequency due to the c-axis length stretched larger which were presumed in accordance with ref[23]. From AFM analysis, the growth mode might be SK mode. The result is different from GaSe deposited by MBE system (layer by layer mode) which belong to VdWE. After the analysis of XRD, Raman spectra and AFM, we find that the behavior is unlike VdWE or quai-VdWE. Hence the lattice mismatch is an important parameter we must consider when we deposit GaSe thin films by pulsed laser deposition.
"Laser pulse duration and electric field effects in the pulsed laser deposition of titanium and silicon carbides." Tulane University, 2007.
Find full textacase@tulane.edu
ALLEN and 許志宇. "The Study of CuInSe2 thin film by the pulse electro deposition." Thesis, 2008. http://ndltd.ncl.edu.tw/handle/98115690491463341324.
Full text吳鳳技術學院
光機電暨材料研究所
96
Abstract This study will use electro-depositing technique to add (Ethylene Diamine Tetraacetic Acid,EDTA) in chloride solution to electrodeposit CuInSe2 thin film on ITO electrode. This major study will to use on the current density, pH value and ion concentration effect on CuInSe2 thin film generation during the deposition. By the design of experiment to control and analysis each factor. Using electro-chemical method to analysis electro-deposition CuInSe2 thin films mechanism and thin film Stoichiometry; crystal grain size and crystal structure. In the CuInSe2 thin film composition analysis one could find the effect of the difference current density on thin film composition. The experimental result shows in addition, deposit current density influence to CIS thin film surface morphological very huge; At the same time the adding amount of EDTA makes up CIS compositions, the size of crystalline grain and surface shape looks also play an important role. This experiment using current density 0.125ASD get a better composition (Cu: In: Se=0.9:1.2:1.9).
Jenderka, Marcus. "Pulsed Laser Deposition of Iridate and YBiO3 Thin Films." Doctoral thesis, 2016. https://ul.qucosa.de/id/qucosa%3A15345.
Full textThe present thesis reports on the thin film growth of ternary oxides Na2IrO3, Li2IrO3, Y2Ir2O7 and YBiO3. All of these oxides are candidate materials for the so-called topological insulator and spin liquid, respectively. These states of matter promise future application in quantum computation, and in magnetic memory and low-power electronic devices. The realization of the thin films presented here, thus represents a first step towards these future device applications. All thin films are prepared by means of pulsed laser deposition on various single-crystalline substrates. Their structural, optical and electronic properties are investigated with established experimental methods such as X-ray diffraction, spectroscopic ellipsometry and resistivity measurements. The structural properties of Na2IrO3 thin films, that were previously realized in the author’s M. Sc. thesis for the first time, are improved significantly by deposition of an intermediate ZnO layer. Single-crystalline Li2IrO3 thin films are grown for the first time and exhibit a defined crystal orientation. Measurement of the dielectric function gives insight into electronic excitations that compare well with single crystal samples and related iridates. From the data, an optical energy gap of about 300 meV is obtained. For Y2Ir2O7 thin films, a possible (111) out-of-plane preferential crystal orientation is obtained. Compared to chemical solution deposition, the pulsed laser-deposited YBiO3 thin films presented here exhibit a biaxial in-plane crystal orientation up to a significantly larger film thickness. From the measured dielectric function, a direct and indirect band gap energy is determined. Their magnitude provides necessary experimental feedback for theoretical calculations of the electronic structure of YBiO3, which are used in the prediction of the novel states of matter mentioned above. After the introduction and motivation of this thesis, the second chapter reviews the current state of the science of the studied thin film materials. The following two chapters introduce the sample preparation and the employed experimental methods, respectively. Subsequently, the experimental results of this thesis are discussed for each material individually. The thesis concludes with a summary and an outlook.
Chen, Kuang-Tze, and 陳光澤. "Electrochemical Study of Sodium Cobalt Oxide Electrode Prepared by Pulsed Laser Deposition." Thesis, 2011. http://ndltd.ncl.edu.tw/handle/44333460642576426168.
Full text國立暨南國際大學
應用化學系
99
In this research, layered sodium cobalt oxide thin film has deposited on two conducting substrates by Pulsed Laser Deposition (PLD). The grown Na0.62CoO2 thin film typically has hexagonal structure with R-3m space group. Problems of lattice mismatch between growth layer and conducting substrate have successfully solved. Crystalline thin film electrode can be produced by adjusting power of laser, substrate temperature and deposition time. The grown thin film electrode exhibits good quality and repeatability for electrochemical experiment. Variations of sodium content and redox reaction on the Na0.62CoO2 have been studied by changing the applied potential on thin film electrode. Ion exchanged of Ag+(aq) for Na+(aq) forms the silver cobalt oxide (AgxCoO2) thin film electrode. The potential dependence of AgxCoO2 stoichiometry is found and demonstrated in this work.
陳世銘. "Preparation and electric characterization of AZO:N/p-Si heterostructure by pulse laser deposition." Thesis, 2009. http://ndltd.ncl.edu.tw/handle/56997482774795463897.
Full textHsu, Wen-Chang, and 許文昌. "A study of gas diffusion layers of Proton Exchange Membrane Fuel Cells modify by pulse electro-deposition." Thesis, 2009. http://ndltd.ncl.edu.tw/handle/72953168921091063754.
Full text逢甲大學
材料科學所
97
In the proton exchange membrane fuel cell (PEMFC), the catalyst layer is the most expensive in all key materials. In order to decrease the cost of fuel cell, it is necessary to use a new electrochemical deposition method to prepare nanoparticle on gas diffusion layers. This experiment was conducted by using pulse electrochemistry deposition method to prepare nano size of pt particle on carbon black of gas diffusion layer for proton exchange membrane fuel cell. The catalyst layer was prepared in 1M H2SO4 +0.002M H2PtCl6 by controlling varying charge time of pulse electro-deposition. After inserting Nafion 117 membrane between two gas diffusion layers and hot pressing the electrodes at 140℃for 90s, the membrane electrode assembly were made for PEMFC testing The Pt loading was between 0.0024 mg/cm2 and 0.0116 mg/cm2 while characterizing the shape and size of the Pt nanoparticles by field-emission scanning electron microscopy and analyzing the amounts of platinum loading by inductively coupled plasma optima optical emission spectrometer. In addition, the platinum crystallization was determined by X-ray powder diffraction analyses. Moreover, the adsorption and desorption reactions of hydrogen with platinum catalysts were analyzed via cyclic voltammograms. A peak current density of 0.0249 A/cm2 could be reached at pulse electro-deposition charge time of 3200s.
Myers, Michelle Anne. "Processing and Characterization of P-Type Doped Zinc Oxide Thin Films." Thesis, 2013. http://hdl.handle.net/1969.1/149354.
Full textAraujo, Roy A. "Metal Nitride Diffusion Barriers for Copper Interconnects." 2008. http://hdl.handle.net/1969.1/ETD-TAMU-2008-12-159.
Full textKu, Chun-Wei, and 古竣偉. "Fabricating Gallium Nitride Epilayer on Zinc Oxide Buffer Layer via Pulsed Laser Deposition System and Opto-electric Properties Analysis." Thesis, 2013. http://ndltd.ncl.edu.tw/handle/h2y3hz.
Full text國立臺灣大學
光電工程學研究所
101
The study of this thesis is to investigate the hydrothermal method for growing high-quality zinc oxide thin film and the homemade pulsed laser deposition system for fabricating high-quality gallium nitride thin film on zinc oxide buffer layer. First, we introduce to obtain high-quality ZnO thin film via hydrothermal method. After that, we use homemade PLD to fabricate high-quality GaN thin film on ZnO buffer layer, and then the effect of nitrogen pressure on properties of GaN thin film is also investigated. In the study of growing high-quality ZnO thin film, the ZnO thin film was successfully fabricated on the p-type GaN epilayer via the hydrothermal method. We successfully used chemical kinetics to simulate the relationship of the growth concentration and the growth time, thus determining the optimal conditions to fabricate the ZnO thin film on a p-type GaN epilayer. Subsequently, we used AFM, EDS, XRD, and Hall measurements to analyze the characteristics of the ZnO thin film. The roughness of the ZnO thin film is determined by AFM to be about 5.46 nm, where there is no other impurity detected in the EDS spectrum. Besides, under the growth temperature of 90°C and the growth concentration of 100mM for 6 hours, the XRD FWHM of ZnO (0001) shows =0.1682°, which is neck and neck with that fabricated by PLD. This means that it is possible to fabricate good quality ZnO thin film via a low cost hydrothermal method and it can be applied in many fields. We have further fabricated n-ZnO layer onto p-GaN layer to fabricate hetero-junction LEDs and successfully achieved a rectifying I-V curve and light emission from current injection. The EL emission of the LED is dominated in the ZnO layer. All results show that the ZnO thin film fabricated by the low-cost hydrothermal method has good potential for possible applications in the industry of light-emitting diodes and take the place of GaN for the material of emitting layer. Next, we use homemade pulsed laser deposition system to epitaxy high-quality gallium nitride thin film on zinc oxide buffer layer. During the deposition process, the high energy plume collides or scatters with nitrogen in atmosphere. This phenomenon greatly affected the crystalline of GaN thin film. The experimental data shows that the properties of GaN thin film fabricate under deposition condition substrate heating temperature 900 oC, laser energy 600mJ/pulsed, 7 Hz laser repetition frequency, and operating nitrogen pressure at 1x10-2 torr are very good. The UV-visible spectrum shows that average transmittance in the visible range is 87 % , and the EDS spectrum reveals that the element ratio of Ga and N is approach to 1:1. The XRD FWHM of the GaN (0002) thin film shows =0.293°, which is neck and neck with that deposited by MOCVD. Furthermore, the surface roughness of the GaN thin film is only 1.6312 nm. It means that this high-quality GaN thin film is also fairly flat.
"Study of indium tin oxide (ITO) thin films prepared by pulsed DC facing-target Sputtering (FTS)." 2000. http://library.cuhk.edu.hk/record=b5890427.
Full textThesis (M.Phil.)--Chinese University of Hong Kong, 2000.
Includes bibliographical references.
Text in English; abstracts in English and Chinese.
by Fung Chi Keung = Cai yong mai chong zhi liu dian yuan dui ba jian she ji shu zhi bei yin xi yang hua wu bo mo de yan jiu / Feng Zhiqiang.
Acknowledgements --- p.i
Abstract --- p.ii
論文摘要 --- p.iii
Table of contents --- p.iv
List of figures --- p.viii
List of tables --- p.xii
Chapter Chapter 1 --- Introduction --- p.1-1
Chapter 1.1 --- Genesis --- p.1-1
Chapter 1.2 --- Aims and Objectives --- p.1-1
Chapter 1.3 --- Layout of Thesis --- p.1-3
References --- p.1-4
Chapter Chapter 2 --- Literature Review --- p.2-1
Chapter 2.1 --- Introduction to transparent conducting oxides (TCOs) --- p.2-1
Chapter 2.2 --- Indium tin oxide (ITO) --- p.2-2
Chapter 2.2.1 --- Use of ITO --- p.2-2
Chapter 2.2.2 --- Structure and properties of ITO --- p.2-3
Chapter 2.3 --- Properties of ITO films deposited by different growth techniques --- p.2-8
Chapter 2.3.1 --- Sputtering --- p.2-9
Chapter 2.3.2 --- Vacuum evaporation --- p.2-11
Chapter 2.3.3 --- Spray pyrolysis --- p.2-11
Chapter 2.3.4 --- Chemical vapor deposition (CVD) --- p.2-12
Chapter 2.3.5 --- Reactive ion plating --- p.2-12
Chapter 2.4 --- Contradictions in existing literature --- p.2-13
References --- p.2-15
Chapter Chapter 3 --- Thin Film Fabrication and Process --- p.3-1
Chapter 3.1 --- Facing-target sputtering (FTS) --- p.3-1
Chapter 3.2 --- Asymmetric bipolar pulsed DC power source --- p.3-3
Chapter 3.2.1 --- Target poisoning --- p.3-3
Chapter 3.2.2 --- Preferential sputtering --- p.3-4
Chapter 3.2.3 --- Discussion --- p.3-4
Chapter 3.3 --- Substrates --- p.3-6
Chapter 3.3.1 --- Microscopic glass --- p.3-7
Chapter 3.3.2 --- Corning 7059 glass --- p.3-8
Chapter 3.3.3 --- Epitaxial growth --- p.3-8
Chapter 3.3.3.1 --- Epitaxial lattice matching --- p.3-8
Chapter 3.3.3.2 --- Yttrium stabilized zirconia (YSZ) --- p.3-9
Chapter 3.3.3.3 --- Sapphire --- p.3-9
Chapter 3.3.3.4 --- Silicon wafer --- p.3-11
Chapter 3.3.4 --- Substrate cleaning --- p.3-11
Chapter 3.4 --- Targets for the reactive sputtering of ITO films --- p.3-13
Chapter 3.4.1 --- Indium Tin Oxide target (90wt% ln203 : 10wt% Sn04) --- p.3-14
Chapter 3.4.2 --- Indium Tin alloy target (90wt% In : 10wt% Sn) --- p.3-14
Chapter 3.5 --- Deposition conditions --- p.3-16
Chapter 3.5.1 --- Sputter atmosphere --- p.3-16
Chapter 3.5.2 --- Deposition pressure --- p.3-16
Chapter 3.5.3 --- Deposition power --- p.3-17
Chapter 3.5.4 --- Target to substrate distance --- p.3-17
Chapter 3.5.5 --- Pulse frequency and pulse width --- p.3-17
Chapter 3.6 --- Deposition --- p.3-17
References --- p.3-19
Chapter Chapter 4 --- Measurement and Analysis Techniques --- p.4-1
Chapter 4.1 --- Resistivity measurement --- p.4-1
Chapter 4.2 --- "Transmittance, reflectivity and absorption measurements" --- p.4-3
Chapter 4.3 --- Thickness measurement --- p.4-4
Chapter 4.4 --- "Crystal structure, surface morphology and roughness measurements" --- p.4-4
Chapter 4.5 --- Photolithography --- p.4-7
Chapter 4.6 --- Hall effect measurements --- p.4-8
References --- p.4-10
Chapter Chapter 5 --- Experimental results and discussions --- p.5-1
Chapter 5.1 --- Effect of O2 partial pressure --- p.5-1
Chapter 5.1.1 --- Deposition rate --- p.5-2
Chapter 5.1.2 --- Electrical and optical properties --- p.5-4
Chapter 5.1.3 --- Structure and orientation --- p.5-16
Chapter 5.1.4 --- Surface morphology and roughness --- p.5-22
Chapter 5.1.5 --- Conclusion --- p.5-29
Chapter 5.2 --- Effect of substrate temperature --- p.5-29
Chapter 5.2.1 --- Electrical and optical properties --- p.5-29
Chapter 5.2.2 --- Structure and orientation --- p.5-44
Chapter 5.2.3 --- Surface morphology and roughness --- p.5-49
Chapter 5.2.4 --- Conclusion --- p.5-54
Chapter 5.3 --- Effect of vacuum annealing --- p.5-54
Chapter 5.3.1 --- Electrical and optical properties --- p.5-54
Chapter 5.3.2 --- Conclusion --- p.5-59
Chapter 5.4 --- Effect of different substrates --- p.5-59
Chapter 5.4.1 --- Comparison of heteroepitaxial and polycrystalline ITO films --- p.5-60
Chapter 5.4.2 --- Conclusion --- p.5-63
Chapter 5.5 --- Effect of film thickness --- p.5-64
Chapter 5.5.1 --- Film thickness calibration --- p.5-64
Chapter 5.5.2 --- Electrical properties --- p.5-64
Chapter 5.5.3 --- Conclusion --- p.5-67
Chapter 5.6 --- Effect of deposition pressure --- p.5-68
Chapter 5.6.1 --- Deposition rate --- p.5-68
Chapter 5.6.2 --- Electrical properties --- p.5-70
Chapter 5.6.3 --- Conclusion --- p.5-70
Chapter 5.7 --- Effect of target pre-conditioning --- p.5-72
Chapter 5.8 --- Conclusion --- p.5-72
References --- p.5-74
Chapter Chapter 6 --- Further works --- p.6-1
Appendix I
Wu, Bo-Hua, and 吳柏樺. "Study of the dye-sensitized solar cells using ZnO/TiO2 core-shelled electrode fabricated by pulse electrochemical deposition of TiO2 on ZnO." Thesis, 2014. http://ndltd.ncl.edu.tw/handle/c57eb8.
Full text國立東華大學
材料科學與工程學系
102
In this study, we coated titanium oxide on the surface of the ZnO particles to form a composite core-shelled structure as an anode for the dye-sensitized solar cells. The solar cell efficiency is successfully enhanced from 1.19% to 1.48% after titanium coating. The efficiency enhancement is accomplished, using titanium di-sulfate solution (Ti(SO4)2) as electrolyte, through the pulsed electrochemical deposition method, which provide appropriate control of thickness of the titanium oxide film that can be coated on the entire interior surface of a mesoporous ZnO film. We found the applied voltage has significant effect on titanium oxide film coated on the ZnO surface by XPS analysis. Under negative bias, the titanium coating rate increases, and the Ti3+ increases relative to Ti4+, with the amount of the applied voltage. Under positive bias, the Jsc increases with the amount of voltage, either due to the modification on the mesoporous surface by acid ligands or by the positive bias itself that turns Ti3+ into Ti4+. We found two most important factors that controls the solar cell efficiency through titanium oxide coating, which are oxygen vacancy (Vo) and film thickness of titanium oxide. The oxygen vacancy is further distinguished into the oxygen vacancy at the ZnO/TiO2 interface, and the oxygen vacancy on the surface of the coated titanium oxide film. We confirmed that the presence of oxygen vacancy at the ZnO/TiO2 interface helps the electronic conduction of the electrode and that the presence of the oxygen vacancy on the surface of the coated titanium oxide film promotes the electron recombination on the titanium oxide surface. As a consequence, the enhancement of the solar cell efficiency should be achieved through, on one hand, the preservation of oxygen vacancy at the ZnO/TiO2 interface and, on the other hand, suppression of the oxygen vacancy on the surface of the coated titanium oxide film. The increase of film thickness of titanium oxide suppresses the electron recombination at the titanium oxide surface, however, at the expense of compromising electronic conduction of the electrode. As a consequence, the thickness should be optimized to achieve highest efficiency of the solar cells. Considering both Vo and thickness factors, we are able to find a titanium oxide coating recipe that promotes the solar cell efficiency. We first coat a titanium oxide film with parameters that contains adequate amount of Ti3+, to assure the conduction of the electron at the ZnO/TiO2 interface. Next we proceed the coating using the same parameters until the targeted thickness is achieved. Finally we coat a thin layer of titanium oxide using parameters denoted as 1d5r to suppress the surface electron recombination as a result of reduced amount of Ti3+ in this coating layer using coating parameters of 1d5r. The reported efficiency enhancement to 1.48% is thus achieved.