Thèses sur le sujet « Impurity doping »
Créez une référence correcte selon les styles APA, MLA, Chicago, Harvard et plusieurs autres
Consultez les 16 meilleures thèses pour votre recherche sur le sujet « Impurity doping ».
À côté de chaque source dans la liste de références il y a un bouton « Ajouter à la bibliographie ». Cliquez sur ce bouton, et nous générerons automatiquement la référence bibliographique pour la source choisie selon votre style de citation préféré : APA, MLA, Harvard, Vancouver, Chicago, etc.
Vous pouvez aussi télécharger le texte intégral de la publication scolaire au format pdf et consulter son résumé en ligne lorsque ces informations sont inclues dans les métadonnées.
Parcourez les thèses sur diverses disciplines et organisez correctement votre bibliographie.
Ciarkowski, Timothy A. « Low Impurity Content GaN Prepared via OMVPE for Use in Power Electronic Devices : Connection Between Growth Rate, Ammonia Flow, and Impurity Incorporation ». Diss., Virginia Tech, 2019. http://hdl.handle.net/10919/94551.
Texte intégralDoctor of Philosophy
GaN is a compound semiconductor which has the potential to revolutionize the high power electronics industry, enabling new applications and energy savings due to its inherent material properties. However, material quality and purity requires improvement. This improvement can be accomplished by reducing contamination and growing under extreme conditions. Newly available bulk substrates with low defects allow for better study of material properties. In addition, very thick films can be grown without cracking on these substrates due to exact lattice and thermal expansion coefficient match. Through chemical and electrical measurements, this work aims to find optimal growth conditions for high purity GaN without a severe impact on growth rate, which is an important factor from an industry standpoint. The proposed thicknesses of these devices are on the order of one hundred microns and requires tight control of impurities.
Zhao, Hehong. « Impurity and Back Contact Effects on CdTe/CdS Thin Film Solar Cells ». Scholar Commons, 2007. https://scholarcommons.usf.edu/etd/580.
Texte intégralErwin. « Electron eigenvalues and eigenfunctions for a nanochannel with a finite rectangular barrier ». Virtual Press, 1994. http://liblink.bsu.edu/uhtbin/catkey/917032.
Texte intégralDepartment of Physics and Astronomy
ANAND, ABHINAV. « Spectroscopic avenues and photophysical phenomena in Colloidal Nanocrystals ». Doctoral thesis, Università degli Studi di Milano-Bicocca, 2021. http://hdl.handle.net/10281/311084.
Texte intégralColloidal semiconductor nanocrystals (NCs), owing to their size-tuneable electronic properties and solution processability, have long been proposed as versatile chemically synthesized alternatives for many photonic, optoelectronic, and quantum computational technologies as well as super-atomic functional building blocks for bottom-up assembled artificial metamaterials. Since their original discovery over 30 years ago, tremendous advancements in colloidal and surface chemistry, NC physics, and device application have brought this vision closer to reality. In this work I explore these photophysical phenomena in four different NC systems diversified by chemical composition and shapes. I studied the most favorable intrinsic ternary CuInS2 NCs which inherently offers heavy metal free, non-toxic alternatives to the existing Cd and Pb based materials with a large Stokes shift and long photoluminescence decay time. The origin of these optical properties in CuInS2 NCs were however not fully understood with conflicting theories describing its characteristic aforementioned properties. Here, subsequential to experimentally confirming the valence band fine structure origin of luminescence in these nanostructures, we utilized the optimized NCs and fabricated a large area Luminescent solar concentrator of 30ˣ30 cm2 area with record Optical Power Efficiency of 6.8% to the date. Then, I discuss the effects of electronic impurity doping in binary chalcogenide NCs synthesized by a novel seeded growth procedure resulting in quantized dopants in each NC thus overcoming the Poissionian bottleneck for their diluted magnetic semiconductor properties. Structural, spectroscopic, and magneto-optical investigations trace a comprehensive picture of the physical processes involved, resulting from the exact doping level of the NCs. Gold atoms, doped here for the first time through the reaction protocol into II−VI NCs, are found to incorporate as non-magnetic Au+ species activating intense size-tuneable intragap photoluminescence and artificially offsetting the hole occupancy of valence band states. Fundamentally, the transient conversion of Au+ to paramagnetic Au2+ (5d9 configuration) under optical excitation results in strong photoinduced magnetism and diluted magnetic semiconductor behaviour revealing the contribution of individual paramagnetic impurities to the macroscopic magnetism of the NCs unlocking their potential to be exploited for applications in quantum and spintronic devices. Moreover, I communicate the effects of substitutional doping with paramagnetic atoms in Manganese doped CsPbCl3 perovskite NCs and reveal a peculiar energy transfer mechanism involving shallow defects states subsequently resulting in dual emission and inducing Stokes shift desirable for photon management technologies. Finally, I conclude by talking about the effect of shape anisotropy in colloidal NC systems by synthesizing and studying two-dimensional colloidal CdTe nanoplatelets. Moreover, I report some very interesting preliminary spectroscopic data that presents these NC systems at great heed with respect to their application in lasing technology and in Ultrafast radiation detection applications. Through the course of my PhD, I worked on the colloidal synthesis of nanostructures, and studied the aforementioned NC systems using structural characterization techniques like X-Ray diffractions and transmission electron microscopy. Spectroscopic techniques including ultrafast transient absorption, steady state and time resolved photoluminescence spectroscopy at cryogenic temperatures, magnetic circular dichroism and electron paramagnetic resonance were used to study and report these nanostructures, thus elucidating their fundamental photophysics and exploit their applicative potential in modern, next generation technologies.
Dürr, Jérôme. « Contribution à l'étude structurale du système BaBiO3 dopé par du plomb ou par du potassium ». Grenoble 1, 1993. http://www.theses.fr/1993GRE10008.
Texte intégralBoukezzata, Messaoud. « Mecanismes d'oxydation des si-lpcvd fortement dopes au bore ». Toulouse 3, 1988. http://www.theses.fr/1988TOU30183.
Texte intégralHénaux, Stéphane. « Contribution à l'amélioration des méthodes de caractérisation électrique des matériaux Silicium Sur Isolant (SOI) ». Université Joseph Fourier (Grenoble), 1998. http://www.theses.fr/1998GRE10116.
Texte intégralDomange, Jocelyn. « Étude et exploitation de bolomètres de nouvelle génération à électrodes concentriques pour la recherche de matière noire froide non-baryonique dans l’expérience Edelweiss II ». Thesis, Paris 11, 2011. http://www.theses.fr/2011PA112169/document.
Texte intégralEDELWEISS is a direct non-baryonic cold dark matter detection experiment in the form of weakly interacting massive particles (also known as WIMPs), which currently constitute the most popular candidates to account for the missing mass in the Universe. To this purpose, EDELWEISS uses germanium bolometers at cryogenic temperature (20 mK approximately) in the Underground Laboratory of Modane (LSM) at the French-Italian border. Since 2008, a new type of detector is operated, equipped with concentric electrodes to optimize the rejection of surface events (coplanar-grid detectors). This thesis work is divided into several research orientations. First, we carried out measurements concerning charge collection in the crystals. The velocity laws of the carriers (electrons and holes) have been determined in germanium at 20 mK in the <100> orientation, and a complete study of charge sharing has been done, including an evaluation of the transport anisotropy and of the straggling of the carriers. These results lead to a better understanding of the inner properties of the EDELWEISS detectors. Then, studies relating to the improvement of the performances were carried out. In particular, we have optimized the space-charge cancellation procedure in the crystals and improved the passive rejection of surface events (β). The fiducial volume of the detectors has been evaluated using two X-ray lines from cosmically activated radionuclides: 68Ge and 65Zn. Lastly, an exhaustive study of the low energy spectra has been carried out, which makes it possible to develop a systematic analysis method for the search of low-mass WIMPs in EDELWEISS
Atmani, Hassane. « Investigations dans le domaine des comportements thermiques de matériaux désordonnés : application au sélénium et aux mélanges Se-Bi à faible concentration en bismuth ». Rouen, 1988. http://www.theses.fr/1988ROUES009.
Texte intégralMarcon, Jérôme. « Simulation numérique de la diffusion de dopants dans les matériaux III-V pour les composants microoptoélectroniques ». Rouen, 1996. http://www.theses.fr/1996ROUES061.
Texte intégralNi, Wei-Shih, et 倪維仕. « Impurity doping effects on the structural, photoluminescent and magnetic properties of ZnS films ». Thesis, 2016. http://ndltd.ncl.edu.tw/handle/52965194317122186527.
Texte intégral國立彰化師範大學
光電科技研究所
104
This study investigates the effect of Co, Mn, and Cu content on the structural, luminescence, and magnetic properties of sol-gel ZnCoS, ZnMnS, and ZnCuS films by x-ray diffraction (XRD), photoluminescence (PL), energy dispersive spectrometer (EDS), atomic force microscopy (AFM), and alternating gradient magnetometer (AGM) measurements. Dependences of optical properties and crystal structure upon Co, Mn, and Cu content were found. In addition, combining with PL, XRD and AGM results, a direct link between the magnetization and defects of sol-gel ZnCoS, ZnMnS, and ZnCuS films was established. Currents through Cu-doped ZnS (ZnCuS)/n-type Si structures were studied. The electrical conduction investigations suggest that the carrier transport behavior is governed by the Poole–Frenkel emission for ZnCuS/n-type Si devices having the low Cu concentration. However, the carrier transport behavior is governed by the thermionic emission for ZnCuS/n-type Si devices having the high Cu concentration. The photoluminescence result revealed that sulfur vacancy (VS) is the origin of conduction behavior conversion. The dependence of VS on the film composition was identified for providing a guide to control the current transport behavior of ZnCuS/n-type Si devices.
Lu, Shih-Han, et 陸詩涵. « The Effects of Impurity Doping on Microstructure and Optical Properties of TiO2 Thin Films ». Thesis, 2013. http://ndltd.ncl.edu.tw/handle/7juzmc.
Texte intégral義守大學
材料科學與工程學系
101
In this study, we prepared TiO2 optical thin film by RF-sputtering method at room temperature and doped with different contents of glass dopants (1wt%, 3wt%, 5wt%, 10wt%, 15wt%, 20wt%). Ar was used as a sputtering gases. TiO2 optical thin films were deposited on glass substrate and the silicon substrate and annealed (550℃, 650℃, 750℃, 850℃) at 90%N2 with 10%H2 atmosphere to discuss the effects of different doping and annealing conduction on the properties of TiO2 films. The results shows that increasing glass dopants are affected crystal structure. The crystal of TiO2 films are changed from anatase phase to amorphous phase as glass dopants were increased. The FE-SEM images showed that annealing temperature affected grain size of the films. Transmittance and refractive index of the films has the opposite results. The 1wt% doping TiO2 thin film has the best transmittance around 85-95% and the 20wt% doping TiO2 thin film has the best refractive index around 2.37-2.41. The densification of TiO2 films can calculated based on the refractive index of the films. The results showed that the TiO2 film with 20wt% doping has the densest structure with porosity around 10.3-13.5%.
曾宇志. « Effects of surface treatment or impurity doping on the optical property and crystal structure of ZnO nanoparticles ». Thesis, 2011. http://ndltd.ncl.edu.tw/handle/86747893765422871256.
Texte intégral國立彰化師範大學
物理學系
99
The effects of surface treatment or impurity doping on the optical property and crystal structure of ZnO nanoparticles, made by sol-gel method, was investigated in this study. We get the properties of ZnO nanoparticles according to observed the result from X-ray diffraction, scanning electron microscope, photoluminescence, Fourier-transform infrared spectroscopy, Raman spectroscopy, and contact angle measurements. It is found that ZnO nanoparticles released from compressive stress after surface modification, and the crystalline size became smaller. In addition, surface modification led to the formation of surface oxygen vacancies and the production of hydroxyl adsorption, that induced ZnO hydrophilic. Li doping led to the increase of the oxygen-vacancy-related defects density in ZnO nanoparticles. In addition, the photoluminescence intensity of Li-doped ZnO is stronger than un-doped ZnO because the decrease in the probability of nonradiative recombination. The intensity of the Ti-doped ZnO diffraction peaks remarkably decreases with increasing Ti content, suggesting the weakened crystallinity. Ti doping also led to the reduced oxygen-vacancy-related defects in ZnO nanoparticles.
Roro, Kittessa Tolessa. « Influence of V and Mn doping on the electrical transport properties of A Cr +1.2 at.% Ga alloy ». Thesis, 2008. http://hdl.handle.net/10210/1360.
Texte intégralImpurity resonance scattering effects are investigated in the Cr-Ga alloy system. This system has a triple point on its magnetic phase diagram where the paramagnetic (P), incommensurate (I) and commensurate (C) spin-density-wave (SDW) states co-exist. Alloying Cr with the nonmagnetic nontransitional element Ga affects the magnetic properties of Cr in a very unique way. In order to investigate the presence of resonant impurity scattering effects in binary Cr-Ga alloys, electrical resistivity measurements were carried out in the temperature range between 6 K and 85 K. The results of the investigation show: • A nonmonotonic increase in the residual resistivity of the Cr-Ga system with an increase in the Ga content, due to the presence of resonant impurity scattering of conduction electrons. • A low-temperature resistivity minimum observed in some of the Cr-Ga alloys, taken as further evidence for the presence of resonant impurity scattering effects on the conduction electrons. The impurity resonance scattering effects on the electrical resistivity of a Cr + 1.2 at.% Ga alloy, doped with V and Mn to tune the Fermi level through the impurity level, are also investigated. The investigation was complemented by thermal expansion and velocity of sound measurements in the temperature range 77 K to 450 K for the Cr + 1.2 at.% Ga alloy only. This specific Ga concentration was chosen to allow for studying resonant scattering effects in both the ISDW and CSDW phases of the system. This is possible because concentration of 1.2 at.% Ga is just above the triple point concentration. Doping with Mn to increase the electron concentration (eA) drives the alloy deeper into the CSDW phase region of the phase diagram, while doping with V, on the other hand, will drive the alloy towards the ISDW phase region. The results of the study are summarized as follows: • Two relatively sharp peaks, attributed to resonant impurity scattering effects, are observed in the curve of the residual resisitivity as a function of dopant concentration in the ISDW phase of the ternary (Cr0.988Ga0.012)1-xVx and (Cr0.988Ga0.012)1-yMny alloy systems. v • At 0 K the (Cr0.988Ga0.012)1-yMny alloy system transforms from the ISDW to the CSDW phase at y ≅ 0.0032, giving a CSDW phase for y > 0.0032. A peak is observed in the residual resistivity at about this Mn content. This peak can then either be ascribed to a jump occurring in the residual resistivity when the CSDW phase is entered from the ISDW phase or to resonant scattering effects. The conclusion is that the peak is rather related to the latter effect. • The resistivity as a function of temperature of the above two ternary alloy series show well-developed or weak minima at low temperatures for some of the samples. This is taken as further evidence of the influence of impurity resonant scattering effects on the resistivity of these alloys. • The resistivity and thermal expansion coefficient of the polycrystalline Cr0.988Ga0.012 alloy of the present study behaves anomalously close to the ISDW-CSDW phase transition temperature and warrant further investigation. The concentration-temperature magnetic phase diagram of the (Cr0.988Ga0.012)(Mn,V) alloy system was constructed from the magnetic transition temperatures obtained from electrical resistivity measurements. Theoretical analysis of the phase diagram was done using the two-band imperfect nesting model of Machida and Fujita. The results show: • A triple point at (0.21 at.% V, 225 K) where the ISDW, CSDW and P phases coexist on the magnetic phase diagram. • The curvature of all three theoretically calculated phase transition lines in the region of the triple point is of the same sign as that observed experimentally. • The theoretical fit is very good for the ISDW-P and ISDW-CSDW phase transition boundaries, while there is some discrepancy for the CSDW-P phase transition line. This may be attributed to the fact that the theory is one dimensional and that it does not include electron-hole pair breaking effects due to impurity scattering and also not effects of changes in the density of states due to alloying.
Dr. A.R.E Prinsloo Prof. H.L. Alberts
Chen, I.-Cherng, et 陳一誠. « A Study on the Sol-Gel Synthesis, Impurity-Doping, and Afterglow and Thermoluminescent Properties of Long Phosphorescent SrAl2O4:Eu,Dy ». Thesis, 2001. http://ndltd.ncl.edu.tw/handle/71948190269204303487.
Texte intégral國立交通大學
應用化學系
89
The effect of impurity doping, photoluminescent, afterglow, and thermoluminescent properties and for long phosphorescent SrAl2O4:Eu2+, Dy3+ (SAED) and some analogous phosphors derived from a sol-gel synthetic route have been investigated. The improvement on phosphorescence intensity and the lengthening of afterglow persistent time has been observed in the SAED phases with the addition of boron or silicon. In order to investigate the photoluminescence, afterglow, defects and the depth energy of the traps, we have measured the X-ray diffraction (XRD) profiles, SEM and DTA/TGA, photoluminescence (PL), afterglow (AG) and thermoluminescence (TL) spectra to characterize the microstructure and luminescent properties that are relevant to the nature of defects present in long afterglow SAED phases. The SAED phases derived from sol-gel route exhibit smaller grain size and poorer crystallinity, as compared to those synthesized by solid-state method. The wavelength of afterglow (lAG) for SAED derived from sol-gel processes was found to be shorter than lAG for those prepared via solid-state route, which was attributed to difference in host crystal field strength for Eu2+. The effect of host compositions on the PL and AG spectra of SAED phases has also been investigated for samples prepared from starting host precursors with different Al/Sr compositions. We found that Sr3Al2O6 dominated in strontium aluminate with the host precursors with Al/Sr < 1; SrAl2O4 was observed in those with 2 < Al/Sr < 3; however, more than 95% of SrAl12O19 was discovered in those with 9 < Al/Sr ≦12. The amount of SrAl2O4 present in the host with various Al/Sr ratios was found to be critical in the determining the afterglow intensity and the afterglow persistent time, as indicated by the AG curves for SAED phases. The coexistence of SrAl12O19 in the SAED host was found to affect the afterglow duration, whereas that of the Sr3Al2O6 phase was found to be independent of the afterglow persistence. The effect of boron and silicon doping in the SAED phosphors was found to not only increase the crystal defects but also enhance the afterglow intensity. The boron-doped SAED (BSAED) sample was observed to exhibit stronger phosphorescence intensity and longer afterglow duration. This observation can be attributed to the non-homogeneous distribution of glassy strontium borates that promotes the reduction of Eu2+ and increases the trap depth energy, as indicated by surface microstructure analysis of BSAED. The twin peaks observed in the afterglow curves for BSAED phases could probably be attributed to two different traps with different depth energies, as compared to one singlet emission observed in the PL spectra. The hole trapping effect due to Dy3+ codoping in SrAl2O4:Eu2+,Dy3+ phase can be effective only when the samples were reduced under a reducing H2/N2 atmosphere at 1,300℃, as indicated by the TL curve analysis. Otherwise, shallow traps will form as that found in SrAl2O4:Eu2+. In addition, the codoping of Nd3+ coactivator in the SrAl2O4:Eu2+,Nd3+ phase indicated that the Nd3+-doping only increases the afterglow intensity, but doesn’t increase the trap depth, which is similar to the shallow traps present in the SrAl2O4:Eu2+ phase. Based on the experimental Hoogenstraaten’s plots, the calculated trap depth energy was found to be 0.57—0.76 eV, 0.43 eV, and 0.18 eV for SrAl2O4:Eu2+0.05,Dy3+0.05,B0.3, SrAl2O4: Eu2+0.05, Dy3+0.05, and SrAl2O4:Eu2+0.05, respectively, as compared to 0.59 — 0.72 eV for BG-300M.manufactured by Nemoto Co. These results indicate the similarity of nature of the trap levels for all strontium aluminate phosphors described in this research.
Sheppard, Leigh Russell Materials Science & Engineering Faculty of Science UNSW. « Defect chemistry and charge transport in niobium-doped titanium dioxide ». 2007. http://handle.unsw.edu.au/1959.4/40542.
Texte intégral