Thèses sur le sujet « Co-crystalline »
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Fasano, Gianluca. « Polymorphism and co-crystalline phases of polymers ». Doctoral thesis, Universita degli studi di Salerno, 2012. http://hdl.handle.net/10556/296.
Texte intégralCrystalline phases are extremely relevant for properties and applications of many polymeric materials. In fact, their amount, structure and morphology constitute the main factors controlling physical properties of fibers, films and thermoplastics and can be also relevant for properties of rubbers and gels. It is also well known that processing and physical properties of polymer-based materials are strongly affected by the occurrence of polymorphism (i.e. the possibility for a given polymer to crystallize in different crystalline forms) and mesomorphism (i.e. the occurrence of “disordered” crystalline phases, characterized by a degree of structural organization that is intermediate between those identifying crystalline and amorphous phases). Different has been the destiny of polymeric co-crystalline forms, i.e. structures were a polymeric host and a low-molecular-mass guest are co-crystallized. Systems composed of solid polymers and of low molecular mass molecules find several practical applications, including advanced applications. In several cases, additives (often improperly referred as guest molecules) are simply dispersed at molecular level in polymeric amorphous phases, although frequently, to reduce their diffusivity, the active molecules are covalently attached to the polymer backbone, either by polymerization of suitable monomeric units or by grafting the active species onto preformed polymers. A more simple alternative method to reduce diffusivity of active molecules in solid polymers and to prevent their self-aggregation consists in the formation of co-crystals with suitable polymer hosts. Polymeric co-crystalline forms are quite common for several regular and stereoregular polymers, like e.g. isotactic and syndiotactic polystyrene (s-PS), syndiotactic poly-p-methyl-styrene, syndiotactic poly-m-methyl-styrene, syndiotactic poly-p-chloro-styrene, syndiotactic poly-p-fluorostyrene, polyethyleneoxide, poly(muconic acid), polyoxacyclobutane, poly(vinylidene fluoride), syndiotactic polymethylmethacrylate. The removal of the low-molecular-mass guest molecules from co-crystals can generate nanoporous-crystalline phases. In this respect, it is worth noting that nanoporous crystalline structures can be achieved for a large variety of chemical compounds: inorganic (e.g., zeolites), metal-organic as well as organic. These materials, often referred as inorganic, metal-organic and organic “frameworks” are relevant for molecular storage, recognition and separation techniques. The removal of the low-molecular-mass guest molecules from polymer co-crystalline forms generates host chain rearrangements, generally leading to crystalline forms that, as usual for polymers, exhibit a density higher than that one of the corresponding amorphous phase. However, in few cases (to our knowledge, up to now only for s-PS), by using suitable guest removal conditions, nanoporous crystalline forms, exhibiting a density definitely lower than that of the corresponding amorphous phases are obtained. Poly-4-methyl-1-pentene isotactic (i-P4MP1) is a polymer characterized by a complex polymorphism and 4 different crystalline forms, some of which are obtainable only by crystallization with solvent, have been described in the literature. Monolithic and highly crystalline aerogels of isotactic poly(4-methyl-pentene-1) (i-P4MP1) have been prepared by sudden solvent extraction with supercritical carbon dioxide from thermoreversible gels. The cross-link junctions of i-P4MP1 gels, depending on the solvent, can be constituted by pure polymer crystalline phases (I or III or IV) or by polymer-solvent co-crystalline phases (for cyclohexane and carbon tetrachloride gels). Gels with co-crystalline phases lead to aerogels exhibiting the denser crystalline form II while all the other considered gels lead to aerogels exhibiting the thermodynamically stable form I. The effect of solvent on the aerogels pore structure and morphology has been also investigated by scanning electron microscopy and N2 sorption measurements. In all cases the areogels present highly porous interconnected structures with macropores and a large heterogeneity of mesopore size but without micro-sized pores. Poly(2,6-dimethyl-1,4-phenylene)oxide (PPO) is a linear regular polymer, which as s-PS has the advantage to be a commercial thermoplastic polymer. PPO exhibits a high free volume or ultrapermeable amorphous phase and has been recognized as a membrane material with high permeation parameters. Although few papers have recognized that PPO crystalline phases can play a role in gas sorption and transport processes, no correlation between the amount or nature of the crystalline phase and guest sorption properties has been reported. This is mainly due to the scarce information available in the literature relative to the crystalline phases of PPO. Crystalline modifications, exhibiting largely different X-ray diffraction patterns, have been obtained for poly(2,6-dimethyl-1,4-phenylene)oxide (PPO), by gel desiccation procedures as well as by solvent-induced crystallization of amorphous films. The choice of the solvent allows controlling the nature of the crystalline phase. Both amorphous and semicrystalline samples of this commercial thermoplastic polymer exhibit a high uptake of large guest molecules (like, e.g., benzene or carbon tetrachloride), both from vapor phases and from diluted aqueous solutions. Surprisingly, the semicrystalline PPO samples present guest solubility much higher than fully amorphous PPO samples. These sorption experiments, as well as density measurements and classical BET experiments, clearly indicate that the obtained PPO crystalline phases are nanoporous. For these thermally stable PPO-based materials exhibiting nanoporous crystalline and amorphous phases, many applications are predictable. Finally, the preparation procedures and the thermal stability of the co-crystalline phase and FTIR and VCD analysis are presented. In particular co-crystalline phases with racemic and non-racemic guest molecules have been prepared and characterized. The experimental data indicates that the PPO/a-pinene co-crystalline form is chiral, i.e. the unit cell includes all right or left handed polymer helices and (1S-(–) or (1R)-(+) a-pinene guest molucules, respectively. [edited by author]
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Ianniello, Graziella. « Polymeric films with co-crystalline and nanoporous crystalline phases : orientations, chirality and possible applications in photonic crystals ». Doctoral thesis, Universita degli studi di Salerno, 2015. http://hdl.handle.net/10556/2015.
Texte intégralPolymers can crystallize in different crystalline forms; polymorphism is the term to indicate this ability. It is known that processing and physical properties of polymer-based materials are strongly affected by the occurrence of ‘‘polymorphism’’ and ‘‘metamorphism’’ (i.e., the occurrence of ‘‘disordered’’ crystalline phases, characterized by a degree of structural organization that is intermediate between those identifying crystalline and amorphous phases). My PhD thesis is focused on the study and on the characterization of polymer films with co-crystalline and nanoporous crystalline phases. Many polymers are able to form co-crystals i.e. molecules of low molecular weight (guest) trapped in the crystalline polymer lattice (host). Over the past two decades it has been observed that some polymers, with co-crystalline phases, such as syndiotactic polystyrene (sPS) and poly (2,6-dimethyl-1,4-phenylene oxide) (PPO) after guest removal can form nanoporous crystalline phases, able to absorb suitable guest molecules also at low activity. During this work, I have studied the possible molecular orientations that may be induced by solvents during cocrystallization process in polymeric films, (chapter 2); the development of chiro optical response, after co-crystallization with temporary chiral guest (chapter 3) and the possibility to realize photonic crystals by using polymers able to form nanoporous crystalline forms (chapter 4). In detail, in chapter 1 the procedure to obtain disordered nanoporous crystalline phases in sPS films and their possible application is reported. This disordered nanoporous crystalline phase rapidly absorb low molecular mass molecules, also from very dilute aqueous solutions. It is known in literature that nanoporous δ form of sPS is also able to absorb ethylene2b and carbon dioxide 2c-d, that have negatively effects for vegetable. Active packaging by nanoporous-crystalline films, based on the removal of molecules generated by the vegetables being detrimental for their preservation 2e, could be complemented by the slow release of antimicrobial molecules, which could be included as guest of the film crystalline cavities. Therefore the preparation of s-PS co-crystalline films that include guests with antimicrobial activity, in particular the carvacrol guest has been studied and reported in chapter 1. The kinetics of release, in variable concentrations of carvacrol in films with different thickness, has been analyzed. It was observed that the location of antimicrobial molecules mainly in the crystalline phase assure a decrease of desorption diffusivity and hence a long-term antimicrobial release. In chapter 2, the study of the possible molecular orientations that can be developed in polymer films able to form cocrystalline phases, are reported. This phenomenon has been observed only for sPS films until now. In particular, in my thesis has been shown that also other polymers, such as poly (2, 6-dimethyl-1, 4-phenylene oxide) (PPO) and poly (L-lactide) (PLLA), able to form co-crystalline phases, can develop orientations during the co-crystallization process with solvents. These orientations can be useful to the structural studies on PPO and PLLA co-crystalline forms. We have also investigated on the shrinkage behaviour developed in syndiotactic polystyrene (sPS) films after cocrystallization procedures leading to co-crystalline phases. High shrinkage values have been measured on sPS d cocrystalline phase showing a crystalline phase orientation. In order to minimize this effect, novel procedures have been developed. Another aspect of my work is focused on the study of chiro optical response of a racemic polymer crystallized with a temporary chiral guest, as reported in chapter 3. In particular, I evaluated the degree of circular polarization of different thickness sPS films, and of the achiral guests, such as azulene and 4-nitroaniline, included in the polymer crystalline phase after guest exchange procedure. These studies have been useful to investigate on the nature of this phenomenon. Finally, in chapter 4, a method to realize a photonic crystal (PhC) with polymeric materials is reported. A PhC is an object composed by two or more materials with different refractive index and an alternated periodicity. The main advantage to use polymers rather than inorganic materials is the ease and the speed to obtain thin films by spin coating and the low cost of materials. In order to realize a photonic crystal, by using thin layers of PPO presenting nanoporous crystalline phase, it has been necessary to characterize amorphous as well as crystalline phases for this purpose. Techniques such as IRRAS and ellipsometry have been used (as reported in section 4.3 of chapter 4). [edited by Author]
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Zhou, Bo. « Synthesis and characterization of crystalline assembly of poly Nisopropylacry-lamide)-co-acrylic acid nanoparticles ». Thesis, University of North Texas, 2004. https://digital.library.unt.edu/ark:/67531/metadc4671/.
Texte intégralWehner, Arno. « Growth and characterization of thin Al2O3 and Ga2O3 films on single-crystalline Ni, Co, and CoGa substrates ». [S.l.] : [s.n.], 2004. http://deposit.ddb.de/cgi-bin/dokserv?idn=971538360.
Texte intégralMaulny, Aurélia. « Preparation and applications in confectionery of co-crystalline sugar products and a novel hydrated form of sucrose ». Thesis, University of Hull, 2003. http://hydra.hull.ac.uk/resources/hull:8067.
Texte intégralHamm, Marc. « Dynamic mean field simulations of liquid crystalline and amorphous (co)polymers : building a model for polymer joining ». Thesis, University of Cambridge, 2003. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.619528.
Texte intégralBerner, Tim, et Klaus-Dieter Becker. « Electrical conductivity relaxation experiments on single crystalline cobalt silicate Co 2 SiO 4 by using impedance spectroscopy ». Universitätsbibliothek Leipzig, 2015. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-186788.
Texte intégralBerner, Tim, et Klaus-Dieter Becker. « Electrical conductivity relaxation experiments on single crystalline cobalt silicate Co 2 SiO 4 by using impedance spectroscopy ». Diffusion fundamentals 12 (2010) 45, 2010. https://ul.qucosa.de/id/qucosa%3A13885.
Texte intégralNanna, Saverio <1985>. « Optimization of molecular and crystalline forms of drugs, agrochemicals, pesticides in relation to activity, bioavailability, patentability and to the fabrication of polymorphs, solvates, co-crystals with green chemistry methods ». Doctoral thesis, Alma Mater Studiorum - Università di Bologna, 2015. http://amsdottorato.unibo.it/7050/1/Nanna_Saverio_Tesi.pdf.
Texte intégralNanna, Saverio <1985>. « Optimization of molecular and crystalline forms of drugs, agrochemicals, pesticides in relation to activity, bioavailability, patentability and to the fabrication of polymorphs, solvates, co-crystals with green chemistry methods ». Doctoral thesis, Alma Mater Studiorum - Università di Bologna, 2015. http://amsdottorato.unibo.it/7050/.
Texte intégralWeiser, Martin [Verfasser], Sannakaisa [Akademischer Betreuer] Virtanen, Sannakaisa [Gutachter] Virtanen et Mathias Christian [Gutachter] Galetz. « Elementary Mechanisms During the Early Stages of Scale Formation on Single Crystalline Co- and Ni-base Superalloys at High Temperatures / Martin Weiser ; Gutachter : Sannakaisa Virtanen, Mathias Christian Galetz ; Betreuer : Sannakaisa Virtanen ». Erlangen : FAU University Press, 2019. http://d-nb.info/1190359588/34.
Texte intégralShan, Haifeng. « Structure development in melt spinning, cold drawing and cold compression of poly(ethylene-co-octene) with different octene content ». Akron, OH : University of Akron, 2006. http://rave.ohiolink.edu/etdc/view?acc%5Fnum=akron1137341440.
Texte intégral"May, 2006." Title from electronic dissertation title page (viewed 10/11/2006) Advisor, James L. White; Committee members, Avraam I. Isayev, Thein Kyu, Darrell H. Reneker, Shing-Chung "Josh" Wong; Department Chair, Sadhan C. Jana; Dean of the College, Frank N. Kelley; Dean of the Graduate School, George R. Newkome. Includes bibliographical references.
Akyildiz, Hasan. « Hydrogen Storage In Magnesium Based Thin Film ». Phd thesis, METU, 2010. http://etd.lib.metu.edu.tr/upload/12612652/index.pdf.
Texte intégralztü
rk Co-Supervisor : Prof. Dr. Macit Ö
zenbas October 2010, 146 pages A study was carried out for the production of Mg-based thin films which can absorb and desorb hydrogen near ambient conditions, with fast kinetics. For this purpose, two deposition units were constructed
one high vacuum (HV) and the other ultra high vacuum (UHV) deposition system. The HV system was based on a pyrex bell jar and had two independent evaporation sources. The unit was used to deposit films of Mg, Mg capped with Pd and Au-Pd as well as Mg-Cu both in co-deposited and multilayered form within a thickness range of 0.4 to 1.5 &mu
m. The films were crystalline with columnar grains having some degree of preferred orientation. In terms of hydrogen storage properties, Mg/Pd system yielded the most favorable results. These films could desorb hydrogen at temperatures not greater than 473 K. The study on crystalline thin films has further shown that there is a narrow temperature window for useful hydrogenation of thin films, the upper limit of which is determined by the intermetallic formation. The UHV deposition system had four independent evaporation sources and incorporated substrate cooling by circulating cooled nitrogen gas through the substrate holder. Thin films of Mg-Cu were produced in this unit via co-evaporation technique to provide concentrations of 5, 10 and 15 at. % Cu. The films were 250-300 nm thick, capped with a thin layer of Pd, i.e. 5-25 nm. The deposition was yielded nanocrystalline or amorphous Mg-Cu thin films depending on the substrate temperature. At 298 K, the films were crystalline, the structure being refined with the increase in Cu content. At 223 K, the films were amorphous, except for Mg:Cu=95:5. The hydrogen sorption of the films was followed by resistance measurements, with the samples heated isochronally, initially under hydrogen and then under vacuum. The resistance data have shown that hydrogen sorption behaviour of thin films was improved by size refinement, and further by amorphization. Among the films deposited, amorphous Mg:Cu=85:15 alloy could absorb hydrogen at room temperature and could desorb it at 223 K (50 º
C), with fast kinetics.
Tabeshian, Ali. « Production and Characterization of Advanced Bulk Metallic Glasses for Hip Implant Applications ». Thesis, Norges teknisk-naturvitenskapelige universitet, Institutt for materialteknologi, 2011. http://urn.kb.se/resolve?urn=urn:nbn:no:ntnu:diva-16351.
Texte intégralIsreb, Abdullah. « The use of solubility parameters to predict the behaviour of a co-crystalline drug dispersed in a polymeric vehicle : approaches to the prediction of the interactions of co-crystals and their components with hypromellose acetate succinate and the characterization of that interaction using crystallographic, microscopic, thermal, and vibrational analysis ». Thesis, University of Bradford, 2012. http://hdl.handle.net/10454/5525.
Texte intégralForster, Maxime. « Compensation engineering for silicon solar cells ». Phd thesis, INSA de Lyon, 2012. http://tel.archives-ouvertes.fr/tel-00876318.
Texte intégralHuang, Gang. « Synthesis and study of crystalline hydrogels, guided by a phase diagram ». Thesis, University of North Texas, 2004. https://digital.library.unt.edu/ark:/67531/metadc4698/.
Texte intégralSong, Mingxia. « Surface plasmon propagation in metal nanowires ». Thesis, Dijon, 2012. http://www.theses.fr/2012DIJOS053/document.
Texte intégralPlasmonic circuitry is considered as a promising solution-effectivetechnology for miniaturizing and integrating the next generation ofoptical nano-devices. The realization of a practical plasmonic circuitry strongly depends on the complete understanding of the propagation properties of two key elements: surface plasmons and electrons. The critical part constituting the plasmonic circuitry is a waveguide which can sustain the two information-carriers simultaneously. Therefore, we present in this thesis the investigations on the propagation of surface plasmons and the co-propagation of surface plasmons and electrons in single crystalline metal nanowires. This thesis is therefore divided into two parts. In the first part, we investigate surface plasmons propagating in individual thick penta-twinned crystalline silver nanowires using dual-plane leakage radiation microscopy. The effective index and the losses of the mode are determined by measuring the wave vector content of the light emitted in the substrate. Surface plasmon mode is determined by numerical simulations and an analogy is drawn with molecular orbitals compound with similar symmetry. Leaky and bound modes selected by polarization inhomogeneity are demonstrated. We further investigate the effect of wire geometry (length, diameter) on the effective index and propagation losses. On the basis of the results obtained during the first part, we further investigate the effect of an electron flow on surface plasmon properties. We investigate to what extend surface plasmons and current-carrying electrons interfere in such a shared circuitry. By synchronously recording surface plasmons and electrical output characteristics of single crystalline silver and gold nanowires, we determine the limiting factors hindering the co-propagation of electrical current and surface plasmons in these nanoscale circuits. Analysis of wave vector distributions in Fourier images indicates that the effect of current flow on surface plasmons propagation is reflected by the morphological change during the electromigration process. We further investigate the possible crosstalk between co-propagating electrons and surface plasmons by applying alternating current bias
Song, Mingxia. « Propagation des plasmons de surface dans des nanofils métalliques ». Phd thesis, Université de Bourgogne, 2012. http://tel.archives-ouvertes.fr/tel-00842236.
Texte intégralКравченко, Володимир Олексійович, Владимир Алексеевич Кравченко et Volodymyr Oleksiiovych Kravchenko. « Фазовий і елементний склад та електрофізичні і магніторезистивні властивості плівкових сплавів на основі Co, Fe та Ni ». Thesis, Вид-во СумДУ, 2011. http://essuir.sumdu.edu.ua/handle/123456789/20820.
Texte intégralДиссертационная работа посвящена изучению закономерностей формирования структуры, фазового состава, электрофизических (удельное сопротивление и температурный коэффициент сопротивления (ТКС)) и магниторезистивных свойств пленочных сплавов CoNi (в интервале концентраций 0<сСо<100 мас.%) и FeNi (cFe=50 мас.%) в интервале толщин 5-200 нм и температур 300-700 К, и магниторезистивных свойств трехслойных пленок на основе этих сплавов. Установлено, что в процессе осаждения пленочных сплавов CoNi испарением готового сплава состав полученной пленки практически совпадает с составом исходного материала, что определяется близостью физических свойств компонент. Для сплава Fe50Ni50 при таком способе осаждения наблюдается обогащение пленок железом. Неотожженные пленки имеют мелкозернистую структуру (размер кристаллитов менее 5-10 нм), в результате отжига размер кристаллитов увеличивается (40-60 нм в случае пленок сплава CoNi, до 30-50 нм для сплава Fe50Ni50). Пленочные сплавы CoNi при содержании Со менее 70 мас.% имеют однофазный состав (ГЦК-твердый раствор), параметр решетки при увеличении содержания Со изменяется в пределах а=(0,352-0,355 нм) в соответствии с правилом Вегарда. При сСо>70 % неотожженным пленкам свойственна ГПУ-решетка, в результате отжига в пленках наблюдается двуфазный состав (ГЦК+ГПУ). Стабильность ГЦК-фазы может быть объяснена снижением температуры фазового перехода для части кристаллитов малого размера за счет фазового размерного эффекта. Для пленок сплава Fe50Ni50 свойственна ГЦК-решетка с параметром а=0,359-0,361 нм. Исследование температурных зависимостей сопротивления пленок показало, что для первого цикла отжига характерно необратимое уменьшение сопротивления, связанное с процессами роста кристаллитов и отжигом дефектов кристаллической структуры. В дальнейших циклах термообработки наблюдается повторение хода температурных зависимостей. Для пленок с эффективной толщиной менее 10 нм характерна экспоненциальная зависимость сопротивления с отрицательными значениями ТКС, что указывает на термически активированную проводимость и связано с образованием структурно и электрически несплошных (островковых) пленок. Показано, что энергия активации проводимости определяется размером островков и промежутков между ними и не зависит от состава сплава. Получена размерная зависимость энергии активации проводимости.Для пленок сплавов CoNi и FeNi с толщинами более 20 нм характерны положительные значения ТКС и квадратичная зависимость удельного сопротивления от температуры, свойственная ферромагнитным металлам и связанная с электрон-магнонным взаимодействием. Изучены размерные зависимости удельного сопротивления и ТКС пленок, на основании которых определены параметры электропереноса в рамках ряда теоретических моделей размерных эффектов электропроводности. В работе проведены исследования зависимости сопротивления однослойных пленочных сплавов от величины напряженности внешнего магнитного поля. Установлено, что для всех исследованных образцов наблюдается анизотропное магнитосопротивление. Для полевых зависимостей магнитосопротивления характерно наличие гистерезиса и экстремумов, что связано с изменением доменной структуры образцов в процессе перемагничивания. Для пленочных сплавов FeNi и CoNi исследованы концентрационные и размерные зависимости. Максимальная величина магнитосопротивления (3,5 % для продольного и 2,5 % для поперечного эффекта) наблюдается для сплавов CoNi при содержании Со 40 мас.%. В работе также показана возможность создания на базе рассмотренных пленочных сплавов трехслойных спин-вентильных систем с гигантским магнитосопротивлением (ГМС). Установлено, что для неотожженых трехслойных пленок CoNi/Cu(Ag)/FeNi, CoNi/Cu(Ag)/Co, FeNi/Cu(Ag)/Со с толщиной немагнитного слоя 3-15 нм наблюдается изотропное магнитосопротивление, что является характерным признаком ГМС. Максимальная амплитуда ГМС (1,1 % при Т=300К и 2 % при Т=150К) получена для системы CoNi/Ag/FeNi с толщиной слоя Ag 4-7 нм. Термическая обработка до температуры 500-700 К приводит к переходу от изотропного к анизотропному магнитосопротивлению, что может быть объяснено нарушением сплошного немагнитного слоя в результате диффузионных процессов. При цитировании документа, используйте ссылку http://essuir.sumdu.edu.ua/handle/123456789/20820
The thesis is devoted to the study of mechanisms of the formation of structure, phase composition, electrophysical and magnetoresistive properties of CoNi film alloys (within the concentration interval 0 < сСо< 100 wt.%) and FeNi (cFe=50 wt.%) within the thickness interval of 5-200 nm and temperature interval of 300-700 К, as well as magnetoresistive properties of three-layer films on the basis of these alloys. Unannealed films have fine-grain structure (crystals size is lower than 5-10 nm). Crystals size increase to 40-60 nm as the result of annealing. CoNi film alloys with the Со content lower than 70 wt.% have one-phase composition (FCCsolid solution). Provided Со content is increased, the lattice parameter will be changed according to the Vergard’s rule. Two-phase content (FCC + HCP lattice) will be observed, provided сСо is more than 70 wt.% within the films that are annealed to 700 К. The FCC lattice with the parameter of а=0,359-0,361 nm is the characteristic of Fe50Ni50 alloy films. The films with the effective thickness up to 10 nm are characterized by the exponential dependence of resistance with the negative values of temperature coefficient of resistance. The dependence indicates thermally activated conductivityand is conditioned by the structural and electrical discontinuous films. The size dependence of the conductivity activation energy is obtain. The films of the CoNi and FeNi alloys with the thicknesses more than 20 nm are characterized by the positive values of temperature coefficient of resistance and the quadratic dependence of resistivity on the temperature. The parameters of electric transfer are being determined on the basis of the theoretical models of the size effects of electric conduction. Concentration and size dependences of FeNi and CoNi film alloy magnetoresistance are studied. The maximum value of magnetoresistance (3,5 % for longitudinal and 2,5 % for transverse effect) is observed for the CoNi films with the Со content of 40 wt.%. It has been determined, that GMR is observed within CoNi/Cu(Ag)/FeNi, CoNi/Cu(Ag)/Co, FeNi/Cu(Ag)/Со unannealed three-layer films with the nonmagnetic layer thickness that equals 3-15 nm. The thermal treatment up to the temperature of 500-700 К leads to the change from GMR to anisotropic magnetoresistance. When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/20820
Forster, Maxime. « Compensation engineering for silicon solar cells ». Phd thesis, INSA de Lyon, 2012. http://hdl.handle.net/1885/156020.
Texte intégralBouet, Gilles. « Etude structurale et analytique de complexes d'halogénures d'éléments 3D : mx ::(2) (M = co,ni,cu ; X = cl,br) et de diverses aldoximes furanniques ». Angers, 1987. http://www.theses.fr/1987ANGE0009.
Texte intégral紀喬崧. « Crystalline Structure and Magnetism of Pd/Fe,Co,Ni bilayers on Al2O3(0001) ». Thesis, 2011. http://ndltd.ncl.edu.tw/handle/09401169035432235063.
Texte intégral國立臺灣師範大學
物理學系
100
This study is separated into two parts: (1) Using oblique deposition to change the surface morphology. (STM measurement) We investigated the corresponding magnetic behavior (MOKE measurement), and the crystalline structure (XRD, EXAFS measurement) in Pd/Fe/Al2O3(0001) system. (2) H2 effect in MOKE, we absorption H2 from 10-3 mbar to 1013 mbar and measured MOKE in Pd/Fe,Co,Ni/Al2O3(0001) systems. In many studies, surface morphology plays an important role in magnetic behavior. They are many methods to change it, like ion-sputtering, different stepped substrate…etc. One of the feasible methods is changing the surface morphology by different deposit angle. In Pd/Fe/Al2O3(0001) system. In normal deposition, Fe atoms were follow the sapphire (0001) growth, and the corresponding magnetic hysteresis loop was almost square, it was isotropy. In oblique deposition, Fe grains were connected to form a 1-dimenstorn ripple structure, and habited interesting magnetic behavior. The easy axis is parallel to the ripples, and the hard axis is perpendicular to the ripples. In easy axis, the magnetic hysteresis loop was also square but the coercivity was much bigger than normal deposition. In hard axis, we could see the obvious uniaxial magnetic anisotropy. Another ideal in this experiment was H2 absorption effect on MOKE. We capped Pd films on the top surface after Fe deposition. There are two reasons for the Pd capping layer, one is to protect Fe films oxidation, the other is Pd can adsorption H2 and the optical of MOKE is changed. key words: oblique deposition, magnetic optical Kerr effect
薛坤仁. « Growth, Crystalline Structure, Thermal Stability and Magnetism of Ni, Co/O-3x3/W(111) ». Thesis, 2012. http://ndltd.ncl.edu.tw/handle/08597723424065667003.
Texte intégralLin, Wen-Chin, et 林文欽. « Growth, crystalline structure and magnetic properties of alloy ultrathin films Co(x)Ni(1-x)/Cu(100) ». Thesis, 2000. http://ndltd.ncl.edu.tw/handle/15923490281900790883.
Texte intégral國立臺灣大學
物理學研究所
88
Magnetic alloy ultrathin films CoxNi1-x/Cu(100) were prepared to characterize its behavior of spin reorientation transition (SRT). With the double check of MEED oscillation and quantitative AES analysis, the composition of the alloy films was determined within an accuracy of ± 0.5 %, which allows us to prepare alloy films in very low Co concentration. So the sensitive effect of alloy composition in crystalline structure, morphology and magnetic properties can be characterized in situ by LEED, I/V-LEED and MOKE. The critical thickness of spin reorientation transition (SRT) in magnetic alloy ultrathin films CoxNi1-x /Cu(100) were 7~8, 9~10, 13~14, 17~18 ML for x = 0, 3, 5.5, 8 % respectively, and for x = 10 %, alloy films always reveal in-plane anisotropy up to 20.6 ML. Despite of the composition induced very different SRT behavior when x £ 10%, the vertical inter-layer distance and the morphology of all the films did not show any significant difference. Comparing with other experimental and theoretical results, it is concluded that the magnetic properties such as magnetic anisotropy were extremely sensitive to the average filling 3d electron in the alloy films.
Xu, Zhong-Yi, et 徐忠義. « Using Side‐chain Attachment Density and Backbone Curvature to Regulate D–A Co-oligomer Crystalline Orientation in Thin Film ». Thesis, 2016. http://ndltd.ncl.edu.tw/handle/f7m7vk.
Texte intégral國立臺灣大學
材料科學與工程學研究所
105
Conducting polymers are important materials in the fabrication of optoelectronic devices. The orientation of the polymer crystalline is critical to achieve high charge carrier mobility and performance in the devices. In general, the edge-on orientation is preferred for utilities of organic field-effect transistors, and the face-on orientation is desired for applications in organic solar cells. However, the detail mechanisms behind the cause of favored crystal orientation of conducting polymers are not clearly understood currently. The systematic studies of molecular design and synthesis for the desired crystal orientation are relatively few present in the literatures. In this research, we design and synthesize eight different co-oligomers, poly(thienoisoindigo-alt-(xoctylthiophene)n, PTInT-xC8, where thienoisoindigo unit (TI) acting as an acceptor is conjugated with thiophene (T) as a donor; n is the number of thiophene in a donor segment, and xC8 denotes the number of n-octyl substituted on thiophenes in a repeat unit. We could tailor the crystal orientation by varying two parameters: (1) side-chain attachment density by changing the number of n-octyl substituents (x) on the thiophenes, and (2) the backbone curvature by changing the number of thiophene (n). The co-oligomers were synthesized successfully via either Stille coupling reaction or direct arylation polycondensation, and were characterized by nuclear magnetic resonance spectroscopy (NMR) for chemical structures, matrix-assisted laser desorption/ionization-time of flight mass spectrometry (MALDI-TOF) for molecular weights, grazing-incidence wide angle X-ray scattering (GIWAXS) for crystalline structures, ultraviolet-visible-near infrared absorption spectroscopy (UV-Vis-NIR) for optical properties and cyclic voltammetry (CV) for band gap determination, thermal gravimetric analysis (TGA) and differential scanning calorimetry (DSC) for thermal properties. The differences among 8 co-oligomers are also studied in details by modeling the molecules by the density functional theory (DFT) calclations. The results indicate that: (1) increasing the number of substituted n-octyl chains (x) on the donor segment of thiophenes while the number of thiophenes (n) is fixed, the polymer backbone will be twisted dramatically as shown by molecular modeling. From the absorption spectra, the relative absorption peak intensity of electrons excited from donor’s HOMO to donor’s LUMO (λ1) is increased while the one symbolized intramolecular transfer (λ2) is decreased. The GIWAXS results also indicate that the π-π stacking distances (dπ-π) in the direction of (010) increase. For example, the dπ-π of PTI2T-0C8 and PTI2T-2C8 are 3.57 Å and 4.83 Å, respectively; the π-π interaction of PTI2T-4C8 is weakened enough that no diffraction peaks could be defined. (2) Increasing the number of thiophene (n) on donor segment while fixing the number of substituted n-octyl chains (x) on thiophenes will distort the backbone due to the increasing freedom of torsion, which shortens the π-conjugation length, and the band gap is increased accordingly. For example, Egsol of PTI2T-2C8, PTI3T-2C8 and PTI4T-2C8 is 1.00, 1.18 and 1.25 eV, respectively; Egfilm is 0.87, 1.14 and 1.20 eV, respectively. The GIWAXS study shows the lamellar distances (d(100)) of PTI3T series are larger than those series of PTI2T and PTI4T. The results are due to the comformation differences between the odd and even number of thiophene (n) in donor segment on the backbone. The even number n gives a centrosymmetric structure whereas the odd number exhibits an axisymmetric configuration. Meanwhile, the steric hindrance of side-chain also influences the packing of polymer backbones. Thus, the centrosymmetric polymers (n = 2 or 4) exhibit the edge-on crystal orientation of long-range order due to the strong π-π interaction. Their orientation will be gradually changed to face-on orientation when the number of side-chains (x) on thiophenes equal to 2 or larger. The change of orientation is far more dramatic for axisymmetric co-oligomerss when the number of side-chains is changed due to the the nonlinear characteristic of backbone which are not suitable for standing on substrate. The edge-on packing is observed for co-oligomers (PTI3T-0C8) without side-chain attached on thiophenes. However, the packing orientation becomes well-ordered face-on with two side-chains added onto the donor segment of thiophenes, and amorphous structure is obtained with adding two more side-chains. The CV results also reveal that most of the PTInT could be used as a p-type semi-conductor materials, and part of the co-oligomers are quiet stable at high temperature with the decomposition temperature as high as 390°C. The outcomes of this research provide pathways for designing and synthesizing conducting polymers with desired crystal orientation for specific optoelectronic device applications.
Wu, Cheng-De, et 吳承德. « Effects of Ceria and Chromia Co-Doped on the Crystalline Structure and Dielectric Properties of Strontium Barium Niobate Ceramics ». Thesis, 2007. http://ndltd.ncl.edu.tw/handle/18561863514718226473.
Texte intégral國立成功大學
資源工程學系碩博士班
95
Strontium barium niobate ( SBN ) ceramic is a good electro-optic material and has been widely used. Although SBN single crystals could be used in wide applications, high cost and difficult fabrication have limited its practical use. For optical applications, a ceramic with almost full density and uniform microstructure is greatly desired. Strontium barium niobate co-doped Ce2O3、Cr2O3 is investigated into the crystalline structure and the dielectric properties. Due to the increase of the quantity of the additive, the a axis is increased, but the c axis is decreased. In the dielectric properties, Tmax and εmax decreased with the increase of the content of Ce2O3、Cr2O3, which is essentially determined by the structural change of the NbO6 units in SBN. The remanent polarization is studied by the Hysteresis loop. Due to the increase of the quantity of the additive, decrease the remanent polarization.
Cheng, Mei-Ling, et 程美玲. « Structure and Free Volume Properties of Semi-crystalline Poly(3-hydroxybutyrate-co-3-hydroxyvalerate) Membranes by Positron Annihilation Lifetime Analysis ». Thesis, 2009. http://ndltd.ncl.edu.tw/handle/12787223919352259340.
Texte intégral元智大學
化學工程與材料科學學系
97
Free volume properties in the amorphous region of a series of poly(3-hydroxybutyrate-co-3-hydroxyvalerate) (PHBV) membranes, which were prepared by cold- and melt-crystallization processes, were investigated using positron annihilation lifetime (PAL) spectroscopy in this study. From the lifetime parameters, the temperature dependence of free volume size, amount, free volume size distribution, and fractional free volume, and the thermal expansion of free volume were discussed. Furthermore, the knee temperature was first observed in the melting process of the crystallized PHBV membranes. It indicated that there was structural transition of polymer chains during melting as the corresponding results observed with in situ FTIR measurement. A model which assumed that amorphous phase was subdivided into mobile and rigid amorphous fractions (MAF and RAF) in the semi-crystalline polymer was considered to interpret the temperature dependence of those free volume properties. The difference of free volume properties among various PHBV membranes was created according to the crystalline structure of the polymer from different thermal history. The polymer crystallized at higher temperatures resulted in higher crystallinities, less free volume amounts and lower fractional free volumes. Based on the crystallization conditions, the effect of the crystallization rate of PHBV polymer was first proposed to explain the thermal expansion coefficients of free volume size. The faster crystallization rate is, the higher thermal expansion coefficient and the larger free volume size at higher measuring temperatures are. Morphological observation of the semi-crystalline polymer by small-angle X-ray scattering (SAXS) indicated that the cold-crystallized membranes showed a much thinner thickness of the repeating lamellar/amorphous layers and most likely higher amount of RAF, which restrained the chain motion, than the melt-crystallized membranes. Larger dispersion of the free volume size of melt-crystallized membranes was observed as a result of the bimodal distribution of the lamellar periodicity and less amount of RAF than that of the cold-crystallized membranes. In conclusion, the relationship between the crystalline structure and the free volume properties within the amorphous phase of PHBV polymer was well established. Free volume size and thermal expansion of the free volume in PHBV membranes were affected by the kinetic of crystallization; comparatively, the total amount of free volume and fractional free volume were determined by the final crystallinity. The size distribution of free volume was associated with the crystalline lamellar structure which was dominated by the crystallization conditions.
Wehner, Arno [Verfasser]. « Growth and characterization of thin Al2O3 and Ga2O3 films on single-crystalline Ni, Co, and CoGa substrates / vorgelegt von Arno Wehner ». 2004. http://d-nb.info/971538360/34.
Texte intégralChiang, Tien-Wei, et 江典蔚. « Observation of Anisotropic Effect of Spin Polarizaton Current in Single Crystalline Co/Fe/MgO Grown on MgO(001)、(011) and (111) ». Thesis, 2004. http://ndltd.ncl.edu.tw/handle/52035307399260824243.
Texte intégral國立中正大學
物理系
92
Experiments have been performed by using series of crystalline Co(500 )/Fe(50 )/MgO(X)/Fe(500 ) films (where X=8、16、25).The samples have prepared by molecular beam epitaxy on MgO(001,011,111) substrates. The hysteresis and magnetoresistance measurements have performed and have found the some meaningful result.They are (1)MR ratios are not found very high and the average values are smaller than 0.2%. (2)The thickness of insulating MgO layer makes a little factor of MR ratio and it shows higher for the sample which has thickness of insulating layer is 25, grown on MgO (111). (3) Intensive anisotropic (4) Inverse tunnel magnetoresistance under some direction of magnetic field indicates some important significant in the present experiment. Inverse tunnel magnetoresistance maybe have relation with polarization of Co. Different MR ratio due to changing of direction of magnetic field means that each place of the surface of sample has different density of state. So Fermi sphere is unsymmetrical and shows the different polarization due to applying magnetic field at different angle. The anisotropic has relation with MgO lattice planes and it has 180∘or 90∘symmetry. The experimental values of MR ratio due to circumrotation of magnetic field, match with cos2θperiod, where as the MR ratio fit with cos4θ period for the sample Co(500 )/Fe(50 )/MgO(8)/Fe(500 )/MgO(001) .
Lee, Chao-hsien, et 李昭賢. « Study of the Microstructure of the Concentric Spherulite of Double Crystalline Poly(3-hydroxybutyrate-co-3-hydroxyvalerate)- Poly(ethylene glycol) Block Copolymers ». Thesis, 2012. http://ndltd.ncl.edu.tw/handle/08266225887593188746.
Texte intégral逢甲大學
纖維與複合材料學系
100
Crystalline-crystalline Poly(3-hydroxybutyrate-co-3-hydroxyvalerate) and Poly(ethylene glycol) block copolymers (PHEGs) were synthesized form PHBV2000 and PEG with different number-average molecular weights. This study focused on the microstructure of the concentric spherulite of double crystalline block copolymers. The crystallization and melting behaviors were studied by a differential scanning calorimeter (DSC). The concentric spherulite morphology was observed with a hot stage polarizing microscope (HSPM). The conformation were investigated by an In-situ Fourier transform infrared spectrometer (In-situ FTIR). The microstructure was probed by small angle x-ray scattering (SAXS). Based on DSC and HSPM studies, two crystallization peaks were observed in the PHEGs during the cooling process, where the high temperature crystallization peak related to the PHBV block and low temperature crystallization peak corresponded to the PEG block, respectively. There was a crystallization exothermic peak in PHEG copolymer under isothermal crystallization conditions. It indicated that PHBV block and PEG block crystallized in the same isothermal crystallization condition. In addition, the concentric spherulite morphology of the PHEG2000, PHEG4000, and PHEG6000 were observed using HSPM. The spherulite growth in the PHEG4000 of PHBV block formed first at 35 ℃, then the PEG block crystallized within confined space between the formerly formed PHBV crystal lamellae. The most stretched PEG chain at the center of the PHBV spherulite may nucleate easily under the enough crystallization time, resulting in the formation of the concentric spherulite. The spherulite growth rate of individual spherulites from the PEG block and PHBV block in PHEGs depends on the crystallization environment. However, the growth rate of the unrestricted PHBV block was faster than that of the confined PHBV block and the growth rate of the confined PEG block was faster than that of the unrestricted PEG block. FTIR and SAXS results showed that the PHBV chains were observed in preferred conformations in the crystalline states during the cooling process at 70 ℃, and then continuously adjusted conformational transition in PEG chain were rearranged to form the crystalline during the isothermal crystallization at 35 ℃. SAXS result, the first growth PHBV spherulite acted as the template for the spherulite growth of the PEG block. In addition, we heated to 70 ℃ for melting the PEG block. The long period (L) and amorphous thickness (la) increased. It was possible that the melting of the PEG block existing in the PHBV crystal lamellae.
Roy, Sounak. « Noble Metal And Base Metal Ion Substituted Ceo2 And Tio2 : Efficient Catalysts For Nox Abatement ». Thesis, 2007. http://hdl.handle.net/2005/584.
Texte intégralBhattacharya, Saurav. « Syntheses Structural Transformations, Magnetism, Ferroelectricity and Proton Conduction of Metal Organic Frameworks (MOF) Compounds ». Thesis, 2015. http://etd.iisc.ernet.in/2005/3546.
Texte intégral