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  • About
  • The Global ETD Search service is a free service for researchers to find electronic theses and dissertations. This service is provided by the Networked Digital Library of Theses and Dissertations.
    Our metadata is collected from universities around the world. If you manage a university/consortium/country archive and want to be added, details can be found on the NDLTD website.
331

Optical properties Of CAD-CAM lithium disilicate glass-ceramic in different firing temperatures and thicknesses

Alqahtani, Nasser January 2016 (has links)
Indiana University-Purdue University Indianapolis (IUPUI), Indiana University School of Dentistry / Background: With the emerging of digital dentistry, IPS e.max® CAD lithium disilicate (LD) glass-ceramic material has become one of the most popular esthetic restorative materials in digital assisted dental esthetic restoration. The mechanical and optical properties of this material have been investigated in several studies. However, there is a lack of information and consensus regarding the optical properties of IPS e.max® LD glass-ceramic materials. Objectives: 1) To investigate the optical properties as translucency parameters (TP), Contrast ratio (CR), light transmissions (Lt) and color changes (CC) between high-translucent (HT) and low-translucent (LT) IPS e.max® CAD LD glass-ceramic materials with different crystalline phases and thickness in different firing stages. 2) To investigate the optical properties as TP, CR, Lt and CC of each translucent (HT and LT) IPS e.max® CAD LD glass-ceramic materials with different crystalline phases and thickness in different firing stages. 3) To determine the mathematical relationships of thicknesses of IPS e.max® CAD LD glass-ceramics materials with TP and Lt. Materials and methods: The total of 120 of shade A2 IPS max CAD samples (HT and LT) were prepared into square shape (15.25 mm X 15.25 mm) and were divided into two main groups according to the material translucency (HT and LT) (n=60). Each main group was further divided into 5 sub-groups according to the thickness (1.00, 1.25, 1.5, 1.75, and 2.00 mm) (n=12). Each thickness group was assigned into three groups based on different crystallization (firing) temperatures (750, 820 °C in single stage heating schedule with 1 second and 10 second holding times, respectively, and 840 °C with two-stage heating schedule (RECOM) (820°C, 840 °C with 10 second and 7 min holding time, respectively) as recommended by manufacturer (n=4). CIEL*a*b*, TP, CR, and Lt were measured and calculated for all samples. Statistical analysis: The effects of the test results were evaluated using 3-way ANOVA with factors for Translucency (HT and LT), Firing Temperature (750, 850, and RECOM) and Thickness (1, 1.25, 1.5, 1.75, and 2), as well as all two-way and three-way interactions among the factors. Pair-wise comparisons were made using Least Significant Differences to control the overall significance level at 5%. Results: The mean irradiance and TP for both HT and LT decrease as the thickness of the samples increases from 1 to 2mm with significant difference between the thickness groups within each material translucency groups (HT and LT) and between both HT and LT. The coefficients of absorption (c) of the two materials were calculated. The effective incidence irradiance when material thickness approaches zero (Ie) was also calculated. There is an unexpected spectral peak shift as the thickness of the samples increases. There is no statistically significant difference in Ie at 750˚C and 820 ˚C between the HT and LT. However, there is a statistically significant higher Ie in HT at the recommended firing temperature as expected. Coefficients of translucency parameter (p) of the materials in various firing temperature were defined and the TP of the material as the thickness approaches zero were calculated (TP0). The TP of the materials is directly correlated to the mean irradiance passing through the samples. There is no statistically significant difference in the TP0 and Ie of the HT and LT groups at the recommended firing temperature. Conclusion: In this project we developed modified Beer-Lambert law to describe the parameters governing the effect of thickness on light transmission in dental ceramic material. We also applied the same equation to describe the translucency parameter. The parameters defined in these equations allow us to compare the optical property of dental ceramic material independent of the thickness of the samples.
332

Excitonic fine structure and nonequilibrium phase transition of the electron-hole system in diamond / ダイヤモンドの励起子微細構造と電子正孔系における非平衡相転移の研究

Hazama, Yuji 23 March 2015 (has links)
京都大学 / 0048 / 新制・課程博士 / 博士(理学) / 甲第18784号 / 理博第4042号 / 新制||理||1582(附属図書館) / 31735 / 京都大学大学院理学研究科物理学・宇宙物理学専攻 / (主査)准教授 中 暢子, 教授 田中 耕一郎, 教授 金光 義彦 / 学位規則第4条第1項該当 / Doctor of Science / Kyoto University / DGAM
333

Defects and Optoelectronic properties of Zinc oxide

Adhikari, Naresh 12 August 2019 (has links)
No description available.
334

Chiroptical properties of cellulose derivatives

Ritcey, Anna Marie January 1987 (has links)
No description available.
335

The electrical and optical characterization of MOCVD grown GaAs: ZnSe heterojunctions /

Rochemont, Pierre de January 1986 (has links)
No description available.
336

Nonlocal Metasurfaces for Active and Multifunctional Wavefront Shaping

Malek, Stephanie Claudia January 2023 (has links)
Metasurfaces are nanostructured interfaces capable of manipulating the phase, amplitude, or polarization of free-space light. ‘Local’ metasurfaces typically control the wavefront shape of spectrally broadband light to generate devices such as flat lenses, holograms, and beam steerers. In contrast, ‘nonlocal’ metasurfaces, such as photonic crystals, support spatially-extended optical modes that govern the transmission or reflection spectrum. Therefore, local metasurfaces typically offer spatial control over incident light but not spectral control, while nonlocal metasurfaces impose spectral but not spatial control. This thesis explores nonlocal dielectric metasurfaces with simultaneous spatial and spectral control such that they shape the wavefront only for spectrally narrowband resonant modes but act like an unpatterned substrate for non-resonant light. These devices are formulated from a rational design scheme based on symmetry arguments. Chapter 1 reviews the theoretical basis for these devices. Chapters 2 and 3 discuss experimental demonstrations of nonlocal wavefront-shaping metasurfaces in the near-infrared and visible wavelength regions, respectively. Our initial experimental demonstrations in the near-infrared in silicon metasurfaces were the first verification of their theoretical proposal. In the visible, experimental results of metasurfaces made of silicon-rich silicon nitride suggest potential applications in transparent displays, augmented reality headsets, and quantum optics. Significantly, our nonlocal metasurfaces form a versatile platform for multifunctional and multicolor meta-optics that shape the wavefront distinctively at several different resonant wavelengths, which we have experimentally demonstrated in both the near-infrared and the visible. Chapters 4 and 5 discuss conceptualization and experimentally demonstration of thermally-tunable nonlocal wavefront-shaping metasurfaces. Reconfigurable photonic devices such as zoom lenses and dynamic holograms have posed a substantial challenge and captured the interest of the optics community. We leverage the enhanced light-matter interaction in our nonlocal wavefront-shaping metasurfaces to realize tunable wavefront-shaping using conventional dielectric materials and standard nanofabrication procedures. The operating principle of these devices is that tuning the refractive index of the device with the thermo-optic effect can align or detune the resonant wavelength of a mode from the wavelength of a narrowband incident light source, and the wavefront is shaped only when the optical resonance is spectrally aligned with the incident light. Experimentally, we have demonstrated nonlocal metasurfaces based on structured germanium thin films whose functionality can be thermally switched between that of two different lenses. The thesis is concluded with a section on future prospects.
337

Design and Development of a Two-Photon Absorption Induced Fluorescence Spectrometer and the Investigation of Nonlinear Optical Properties of Organic Chromophores / Aufbau und Entwicklung eines Zwei-Photonen-Absorptions-induzierten Fluoreszenzspektrometers und Untersuchung der nichtlinearen optischen Eigenschaften organischer Chromophore

Michail, Evripidis January 2021 (has links) (PDF)
Main objectives of the present dissertation can be divided in two parts. The first part deals with setting up a spectroscopic technique for reliable and accurate measurements of the two-photon absorption (2PA) cross section spectra. In the second part, this firmly established experimental technique together with conventional spectroscopic characterization, quantum-chemical computations and theoretical modelling calculations was combined and therefore used as a tool to gain information for the so-called structure-property relationship through several molecular compounds. / Die Hauptziele der vorliegenden Dissertation lassen sich in zwei Teile gliedern. Der erste Teil befasst sich mit dem Aufbau einer spektroskopischen Technik zur zuverlässigen und genauen Messung der Zwei-Photonen-Absorptionsquerschnittsspektren (2PA). Im zweiten Teil wurde diese fest etablierte experimentelle Technik zusammen mit konventioneller spektroskopischer Charakterisierung, quantenchemischen Berechnungen und theoretischen Modellrechnungen kombiniert und damit als Werkzeug genutzt, um über mehrere molekulare Verbindungen Informationen für die sogenannte Struktur-Eigenschafts-Beziehung zu gewinnen.
338

Picosecond degenerate four-wave mixing in semiconductors

Canto, Edesly J. 05 1900 (has links)
This study reports on a variety of experimental and theoretical studies conducted in ZnSe, CdTe, and in semiconductor-doped glasses. The transient picosecond degenerate four-wave mixing (DFWM) experiments performed in these II-VI direct-gap semiconductors are part of our efforts to understand the picosecond dynamics of the free-carriers generated via two and three-photon absorption.
339

Optical and Magnetic properties of nanostructures

Nayyar, Neha 01 January 2014 (has links)
In this thesis, Density Functional Theory and Time-Dependent Density-Functional Theory approaches are applied to study the optical and magnetic properties of several types of nanostructures. In studies of the optical properties we mainly focused on the plasmonic and excitonic effects in pure and transition metal-doped noble metal nanochains and their conglomerates. In the case of pure noble metal chains, it was found that the (collective) plasmon mode is pronounceable when the number of atoms in the chain is larger than 5. The plasmon energy decreases with further with increasing number of atoms (N) and is almost N-independent when N is larger than 20. In the case of coupled pure chains it was found that the plasmon energy grows as square root of the number of chains, and reaches the visible light energy 1.8eV for the case of three parallel chains. Doping of pure Au chains with transition-metal atoms leads in many cases to formation of additional plasmon peaks close in energy to the undoped chain peak. This peak comes from the local charge oscillations around the potential minima created by the impurity atom. The effect is especially pronounced for Ni-doped chains. In the multiple-chain case, we find an unusual hybridization of the two different (local and collective) plasmon modes. Changing the chain size and chemical composition in the array can be used to tune the absorption properties of nanochains. The case of coupled finite (plasmonic) and infinite (semiconductor, excitonic) chains was also analyzed. We find that one can get significant exciton-plasmon coupling, including hybridized modes and energy transfer between these excitations, in the case of doped chains. The impurity atoms are found to work as attraction centers for excitons. This can be used to transform the exciton energy into local plasmon oscillations with consequent emission at desired point (at which the impurity is located). In a related study the optical properties of single layer MoS2 was analyzed with a focus on the possibility of ultrafast emission, In particular, it was found that the system can emit in femto-second regime under ultrafast laser pulse excitations. Finally, we have studied the magnetic properties of FeRh nanostructures to probe whether there is an antiferromagnetic to ferromagnetic transition as a function of the ratio of Fe and Rh atoms, as in the bulk alloy.. Surprisingly, the ferromagnetic phase is found to be much more stable for these nanostructures as compared to the bulk, which suggests that band-type effects may be responsible for this transition in the bulk, i.e. the transition cannot be described in terms of modification of the Heisenberg model parameters.
340

Experimental And Theoretical Study Of The Optical Properties Of Semiconductor Quantum Dots

Nootz, Gero 01 January 2010 (has links)
The aim of this dissertation is to gain a better understanding of the unique electronic structure of lead salt quantum dots (QDs) and its influences on the nonlinear optical (NLO) properties as well as the time dynamics of the photogenerated charge carriers. A variety of optical techniques such as Z-scan, two-photon excited fluorescence and time-resolved pump probe spectroscopy are used to measure these properties. The one-photon as well as the degenerate and nondegenerate two-photon absorption (2PA) spectra are measured and the electronic wave functions from a four-band envelope function formalism are used to model the results. We observe local maxima in the 2PA spectra for QD samples of many different sizes at energies where only 1PA is predicted by the model. This is similar to the previously measured transitions in the 1PA spectra which are not predicted by the model but accrue at the energies of the two-photon allowed transitions. Most importantly we observe 2PA peaks for all samples at the energy of the first one-photon allowed transition. This result can only be understood in terms of symmetry breaking and therefore is strong evidence that other transitions, not predicted by the model if the selection rules are left intact, also have the origin in the lifted spatial symmetry of the wave functions. On the other hand, the uniquely symmetric eigenenergies of these quantum-confined energy states in the conduction and valance bands explain the observed trend toward larger two-photon cross-sections as the quantum confinement is increased in smaller QDs. Moreover, this unique feature is shown to reduce the possible relaxation channels for photoexcited carriers, which is confirmed experimentally by the reduced carrier relaxation rate as compared to CdSe QDs which lack this symmetry. Carrier multiplication (CM), a process in which several electrons are excited by the iv absorption of a single photon is studied in PbS QDs. We show that for PbS QDs with radius smaller than 2.5 nm the parameters of CM get very close to the theoretical optimum. Nextgeneration solar cells operating under these ideal conditions could potentially have conversion efficiency of up to 42%. This compares favorably to the 30% efficiency limit of a single junction silicon solar cell.

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