Dissertations / Theses on the topic 'Ferrites spinel'
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Phillips, Peter John. "Conduction processes in spinel ferrites." Thesis, University of Warwick, 1991. http://wrap.warwick.ac.uk/108772/.
Full textPrice, Sean. "Critical and magnetic behaviour of some spinel ferrites." Thesis, University of Portsmouth, 1991. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.304578.
Full textVestal, Christy Riann. "Magnetic couplings and superparamagnetic properties of spinel ferrite nanoparticles." Diss., Available online, Georgia Institute of Technology, 2004:, 2004. http://etd.gatech.edu/theses/available/etd-06072004-131405/unrestricted/vestal%5Fchristy%5Fr%5F200405%5Fphd.pdf.
Full textSong, Qing. "Size and Shape Controlled Synthesis and Superparamagnetic Properties of Spinel Ferrites Nanocrystals." Diss., Georgia Institute of Technology, 2005. http://hdl.handle.net/1853/7645.
Full textBonholzer, Michael. "Magnetic Tunnel Junctions based on spinel ZnxFe3-xO4." Doctoral thesis, Universitätsbibliothek Leipzig, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-212756.
Full textHan, Man Huon. "Development of synthesis method for spinel ferrite magnetic nanoparticle and its superparamagnetic properties." Diss., Atlanta, Ga. : Georgia Institute of Technology, 2008. http://hdl.handle.net/1853/26465.
Full textCommittee Chair: Z. John Zhang; Committee Member: Angus Wilkinson; Committee Member: C P Wong; Committee Member: E. Kent Barefield; Committee Member: Mostafa El-Sayed. Part of the SMARTech Electronic Thesis and Dissertation Collection.
Mercier, Adrien. "Contribution à l'étude et à la réalisation de composants magnétiques monolithiques réalisés par PECS/SPS et à leurs applications en électronique de puissance." Thesis, Université Paris-Saclay (ComUE), 2016. http://www.theses.fr/2016SACLN057/document.
Full textThe increase in switching frequency of power supply induces new problems for the components. These components are active or passive, it is necessary to control the losses so that efficiency remains acceptable. The thesis deals with the study and production of a new transformer structure intended to be part of a switching power supply. These transformers are produced using PECS/SPS method, which is a sintering technology. This technology can be sintered ferrite around the primary and secondary windings. It follows that the components are monolithic.A first part presents the state of the art, and magnetism in the matter. It follows a chapter dedicated to the manufacture of magnetic materials used in the thesis : the ferrites.A second part concerns the ferrites produced by the PECS / SPS process. Firstly, the magnetocrystalline anisotropy of these materials is studied, and it is possible to decrease it by varying the chemical composition. In a second stage, other variables such as the permeability or the polarization are measured, always depending on the chemical composition. The main results show that the sintering by PECS / SPS method is more reducing than conventional sintering, which degrades certain properties such as the resistivity of the ferrites. The last chapter is dedicated to the realization of monolithic processors. A detailed manufacturing protocol is presented.A third part shows the operation of the realized transformers. The usual measurements allow identifying self, mutual and leakage inductances. The values of these inductances show that it is better to use components made not as a transformer, but as a coupler. Finally a converter based on a VRM structure is realized. The switching frequency is 2 MHz, the efficiency is greater than 90%, and the power density is 15 kW / liter
Moura, Alysson Elson Galv?o de. "S?ntese, sinteriza??o e caracteriza??o de ferritas ? base de Ni-Zn." Universidade Federal do Rio Grande do Norte, 2008. http://repositorio.ufrn.br:8080/jspui/handle/123456789/17599.
Full textConselho Nacional de Desenvolvimento Cient?fico e Tecnol?gico
Were synthesized different ferrites NixZn1-xFe2O4 (0,4 ≤ x ≤ 0,6) compositions by using citrate precursor method. Initially, the precursors citrates of iron, nickel and zinc were mixed and homogenized. The stoichiometric compositions were calcined at 350?C without atmosphere control and the calcined powders were pressed in pellets and toroids. The pressed material was sintered from 1100? up to 1200?C in argon atmosphere. The calcined powders were characterized by XRD, TGA/DTG, FTIR, SEM and vibrating sample magnetometer (VSM). All sintered samples were characterized using XRD, SEM, VSM and measurements of magnetic permeability and loss factor were obtained. It was formed pure ferromagnetic phase at all used temperatures. The Rietveld analyses allowed to calculate the cations level occupation and the crystallite size. The analyses obtained nanometric crystals (12-20 nm) to the calcined powder. By SEM, the sintered samples shows grains sizes from 1 to 10 μm. Sintered densities (ρ) were measured by the Archimedes method and with increasing Zn content, the bulk density decrease. The better magnetization results (105-110 emu/g) were obtained for x=0,6 at all sintering temperatures. The hysteresis shows characteristics of soft magnetic material. Two magnetization processes were considered, superparamagnetism at low temperature and the magnetic domains formation at high temperatures. The sintered toroids presents relative magnetic permeability (μr) from 7 to 32 and loss factor (tanδ) of about 1. The frequency response of toroids range from 0,3 kHz to 0,2 GHz. The composition x=0,5 presents both greater μr and tanδ values and x=0,6 the most broad range of frequency response. Various microstructural factors show influence on the behavior of μr and tanδ, such as: grain size, porosity across grain boundary and inside the grain, grain boundary content and domain walls movement during the process of magnetization at high frequency studies (0,3kKz 0,2 GHz)
Foram sintetizadas diferentes composi??es da ferrita Ni1-xZnxFe2O4 com 0,4 ≤ x ≤ 0,6 pelo uso do m?todo dos citratos precursores. Para se obter a fase estequiom?trica do sistema Ni1-xZnxFe2O4 foram misturados e homogeneizados os citratos precursores de ferro, n?quel e zinco. As composi??es estequiom?tricas foram calcinadas em atmosfera ambiente na temperatura de 350?C e depois prensadas em pastilhas e tor?ides. As amostras prensadas foram sinterizadas nas temperaturas de 1100?, 1150? e 1200?C em atmosfera de arg?nio. Os p?s calcinados foram caracterizados por DRX, TGA/DTG, FTIR, MEV e magnetometria de amostra vibrante (MAV) e as amostras sinterizadas por DRX, MEV, MAV, massa espec?fica e medidas de permeabilidade e perdas magn?ticas. Observou-se a forma??o de fase pura ferrimagn?tica em todas as temperaturas aplicadas. A an?lise pelo m?todo de Rietveld calculou o n?vel de ocupa??o dos c?tions e o tamanho de cristalito. Foram obtidos tamanhos de cristais nanom?tricos, de 12 a 20 nm para os p?s calcinados. Por MEV, as amostras sinterizadas apresentam tamanhos de gr?os na faixa de 1 a 10 μm. A massa espec?fica (ρ) do material sinterizado apresenta uma tend?ncia de diminui??o com a adi??o de Zn. Os melhores resultados de magnetiza??o foram obtidos para x=0,6 nas tr?s temperaturas de sinteriza??o, variando de 105 a 110 emu/g. As histereses mostram um perfil de materiais magn?ticos moles. Dois processos de magnetiza??o foram considerados, o superparamagnetismo a baixa temperatura (350?C) e a forma??o de dom?nios magn?ticos em altas temperaturas. Os materiais sinterizados apresentam permeabilidade (μ) de algumas unidades, de 7 a 30, e perdas magn?ticas (tanδ) por volta de 1. A resposta em freq??ncia dos n?cleos toroidais est? na faixa de 0,3 kHz a 0,2 GHz. Os maiores valores de μ e tanδ s?o para x=0,5 e a maior faixa de resposta em freq??ncia ? para x=0,6. V?rios fatores da microestrutura contribuem para o comportamento das grandezas μ e tanδ, tais como: os tamanhos dos gr?os, porosidade inter e intragranular, quantidade de contornos de gr?os e os aspectos da din?mica das paredes de dom?nios quando excitadas magneticamente sob alta freq??ncia
Scarberry, Kenneth Edward. "Biomedical applications of cobalt-spinel ferrite nanoparticles for cancer cell extraction and drug delivery." Diss., Georgia Institute of Technology, 2009. http://hdl.handle.net/1853/33951.
Full textMarija, Milanović. "Sinteza i karakterizacija nanočestičnih prahova na bazi cink-ferita." Phd thesis, Univerzitet u Novom Sadu, Tehnološki fakultet Novi Sad, 2010. https://www.cris.uns.ac.rs/record.jsf?recordId=82019&source=NDLTD&language=en.
Full textThis thesis presents the results of the investigation of the structural and magnetic properties of nanostructured zinc ferrites, ZnFe2O4 and zinc ferrites supstituted with different amount of indium and yttrium, Zn1-xInxFe2O4 and ZnYxFe2-xO4 (0 ≤ x ≤ 0,6). Powders based on zinc ferrites were synthesised by a low temperature wet-chemical method – coprecipitation. The main purpose of this thesis was to establish the relationship between the synthesis, dopants, structure and properties of zinc ferrite based materials. Nanoparticles of ZnFe2O4 were calcined at different temperatures in order to elucidate the influence of the particle size on the magnetic properties of the obtained nanoparticles. In addition, we have investigated the effect of dopant addition on cation distribution in spinel structure, in order to modify the magnetic properties and to obtain the magnetic ceramics with improved properties compared to the bulk-counterparts. The results of X-ray and TEM analyses confirmed the nanosized nature and spinel type structure of the investigated samples. Raman and Mössbauer spectroscopy studies implied on the possible cation distribution between the tetrahedral and octahedral sites and formation of the partially inversed spinel. The study of the magnetic properties showed that hysteresis loops do not saturate even in the presence of high magnetic fields, which confirmed the superparamagnetic and single domain nature of the samples. These observations imply that, besides the particle size, doping (e.g. yttrium and indium) causes significant structural rearrangements which in turn induce changes in magnetic behavior of the investigated nanoparticulate systems.
Bezerra, Maria Jos? Oliveira da Silva. "S?ntese e caracteriza??o da ferrita de MnZn obtida pelo m?todo dos citratos precursores." Universidade Federal do Rio Grande do Norte, 2007. http://repositorio.ufrn.br:8080/jspui/handle/123456789/17778.
Full textConselho Nacional de Desenvolvimento Cient?fico e Tecnol?gico
It was synthesized MnZn ferrite with general formulae Mn1-xZnxFe2O4 (mol%), 0,3 ≤ x ≤ 0,7 by using the citrate precursor method. The precursors decomposition was studied by thermogravimetric analysis (TGA), differential thermogravimetric analysis (DTG), differential thermal analysis (DTA) and Fourier transform infrared (FTIR) of powder calcined at 350?C/3,5h. X-ray diffraction pattern (XRD) of samples was done from 350 to 1200?C/2h using various atmospheres. The power calcined at 350?C/3,5h formed spinel phase. It is necessary atmosphere control to avoid secondary phase such as hematite. From 900 to 1200?C was obtained 90,66 and 100% of MnZn spinel ferrite phase, respectively. Analysis by dispersive energy scanning (EDS) at 350?C shows high Mn and Zn dispersion, indicating that the diffusion process was homogeneous. Semi-quantitative analysis by EDS verified that despite the atmosphere control during calcinations at high temperatures (< 800?C) occurred ZnO evaporation causing stoichiometric deviation. Vibrating sample magnetometer (VSM) measures show soft ferrite material characteristics with Hc from 6,5 x 10-3 to 11,1 x 10-2 T. Saturation magnetization (Ms) and initial permeability (?i) of MnZn spinel phase obtained, respectively, from 14,3 to 83,8 Am2/kg and 14,1 to 62,7 (Am2/kg)T
Foi sintetizada ferrita de MnZn com f?rmula geral Mn1-xZnxFe2O4 (mol%) para 0,3 ≤ x ≤ 0,6 com uso do m?todo dos citratos precursores. A decomposi??o dos precursores foi estudada por an?lise termogravim?trica (TGA), termogravim?trica diferencial (DTG), an?lise t?rmica derivada (DTA) e espectroscopia na regi?o do infravermelho (FTIR) dos p?s calcinados em 350?C/3,5h. Foram feitas difra??es de raios X (DRX) entre 350 e 1200?C/2h usando v?rias atmosferas. O p? calcinado a 350?C/3,5h formou fase espin?lio. ? necess?rio o controle da atmosfera para evitar fases secund?rias como a hematita. Em 900 e 1200?C foram obtidos respectivamente, 90,7 e 100% de fase ferrita espin?lio. An?lises por espectroscopia de energia dispersiva (EDS) em 350?C mostrou alta dispers?o de Mn e Zn, indicando que o processo de difus?o foi homog?neo. A an?lise semi-quantitativa por EDS verificou que apesar do controle da atmosfera durante a calcina??o em altas temperaturas (> 800?C), ocorreu vaporiza??o de ZnO causando desvio estequiom?trico. Medidas por magnet?metro de amostra vibrante (MAV) mostraram caracter?sticas de materiais magneticamente macios com Hc de 6,5 x 10-3 at? 11,1 x 10-2 T. A magnetiza??o de satura??o e a permeabilidade inicial da fase espin?lio de MnZn foi obtida entre 14,3 a 83,8 Am2/kg e 14,1 a 62,7 (Am2/kg)T, respectivamente
Silva, Jos? Eves Mendes da. "S?ntese an?lise das propriedades magn?ticas da ferrita de NiMg e caracter?sticas de absor??o de radia??o." Universidade Federal do Rio Grande do Norte, 2008. http://repositorio.ufrn.br:8080/jspui/handle/123456789/17600.
Full textCoordena??o de Aperfei?oamento de Pessoal de N?vel Superior
It was synthesized different Ni1-xMgxFe2O4 (0,2 ≤ x ≤ 0,7) compositions by use of citrate precursor method. Initially, the precursory citrates of iron, nickel and magnesium were mixed and homogenized. The stoichiometric compositions were calcined from 350?C to 1200?C at ambient atmosphere or in argon atmosphere. The calcined powders were characterized by XRD, TGA/DTG, FTIR, magnetic measures and reflectivity using the wave guide method. I was observed pure magnetic phase formation between 350?C and 500?C, with formation of ferrite and hematite after 600?C at ambient atmosphere. The calcined powder at argon atmosphere formed pure ferromagnetic phase at 1100?C and 1200?C. The Rietveld analyses calculated the cations level occupation and the crystallite size. The analyses obtained nanometric crystals (11-66 nm), that at 900?C/3h presents micrometric sizes (0,45 - 0,70 Om). The better magnetization results were 54 Am2/Kg for x= 0,2 composition, calcined at 350?C/3h and 30 min, and 55,6 Am2/Kg for x= 0,2 1200?C, calcined in argon. The hysteresis shows characteristics of soft magnetic material. Two magnetization processes were considered, superparamagnetism at low temperature and the magnetic domains formation at high temperatures. The materials presented absorption less or equal the 50 % in ranges specific frequency. As for the 2,0 and 3,0 thickness (in 11,0 - 11,8 GHz), the reflectivity of the x= 0,3, 0,5 and 0,4 compositions, all calcined at 900?C/3h showed agreement with MS and O. Various factors contribute for the final radiation absortion effect, such as, the particle size, the magnetization and the polymer characteristics in the MARE composition. The samples that presented better magnetization does not obtaining high radiation absorption. It is not clear the interrelaction between the magnetization and the radiation absorption in the strip of frequencies studied (8,2 - 12,4 GHz)
Foram sintetizadas diferentes composi??es da ferrita Ni1-xMgxFe2O4 com (0,2 ≤ x ≤ 0,7) pelo uso do m?todo dos citratos precursores. Para se obter a fase estequiom?trica Ni1-xMgxFe2O4, inicialmente foram misturados e homogeneizados os citratos precursores de ferro, n?quel e magn?sio. As composi??es estequiom?tricas foram calcinadas entre as temperaturas de 350?C e 1200?C, em atmosfera ambiente ou de arg?nio. Os p?s calcinados foram caracterizados por DRX, TGA/DTG, FTIR, medidas magn?ticas e refletividade pelo m?todo de guia de ondas. Foi observada a forma??o de fase pura ferrimagn?tica entre 350?C e 500?C, formando ferrita e hematita ap?s 600?C, em atmosfera ambiente. O p? calcinado em atmosfera de arg?nio formou fase ferrimagn?tica pura em 1100?C e 1200?C. A an?lise pelo m?todo de Rietveld calculou o n?vel de ocupa??o dos c?tions e o tamanho de cristalito. A an?lise obteve tamanhos de cristais nanom?tricos, (11 - 66 nm), que a 900?C/3h apresentam tamanhos microm?tricos (0,45 0,70 Om). Os melhores resultados de magnetiza??o foram 54 Am2/Kg para a composi??o x= 0,2, calcinada a 350?C/3h e 30 min, e 55,6 Am2/Kg para x= 0,2 a 1200?C, calcinada em arg?nio. As histereses mostraram um perfil de materiais magn?ticos moles. Dois processos de magnetiza??o foram considerados, o superparamagnetismo a baixa temperatura e a forma??o de dom?nios magn?ticos em altas temperaturas. Os materiais apresentaram absor??o igual ou inferior a 50 % em faixas de freq??ncias espec?ficas. Para as espessuras 3,0 e 2,0 mm (em 11-11,8 GHz), as refletividades das composi??es x= 0,3, x= 0,5 e x= 0,4, todas a 900?C/3h demonstraram concord?ncia com MS e O. V?rios fatores contribuem para o efeito final de absor??o de radia??o, tais como, o tamanho de part?culas, a magnetiza??o, e as caracter?sticas do pol?mero na composi??o do MARE. As amostras que apresentaram maiores magnetiza??es n?o atingiram alta absor??o de radia??o. N?o ficou esclarecido a interrela??o entre a magnetiza??o e a absor??o de radia??o na faixa de freq??ncia estudada (8,2 12,4 GHz)
Sabo, Daniel E. "Novel synthesis of metal oxide nanoparticles via the aminolytic method and the investigation of their magnetic properties." Diss., Georgia Institute of Technology, 2012. http://hdl.handle.net/1853/50122.
Full textAbdul, Latiff Hawa Alima Binti. "Magnetic anisotropy and coercivity of tetragonally distorted spinel ferrite particles via the Jahn-Teller distortion and the magnetoelastic coupling." Thesis, Université Grenoble Alpes (ComUE), 2019. http://www.theses.fr/2019GREAY005.
Full textThis study proposes the idea of the so-called tetragonal ferrite magnets by rendering the crystal symmetry of the cubic spinel ferrites to enhance the magnetic anisotropy (and hence, enhance the coercivity). To realize this idea, we synthesized tetragonally distorted (Cu,Co)-ferrite particles and systematically characterized the magnetic properties accordingly with their lattice distortions. The intrinsic and extrinsic factors contributing to coercivity were investigated. To elucidate the magnetic anisotropy, we demonstrated a physical coupling model of the Jahn-Teller (JT) effect and the magnetoelastic (ME) effect within the phenomenological theory. Then, we performed coercivity analysis within two general models of coercivity to clarify the microstructure parameters contributing to the magnetization reversal mechanism. From the magnetoelastic model analysis, we demonstrated the linear expression of the magnetic anisotropy using the tetragonal parameter obtained from the JT distortion. The magnetoelastic coefficient values for Cu (B1Cu = 2 MJ/m3) and Co (B1Co = 40 MJ/m3) deduced from the experimental curve were agreeable with the value calculated for bulk copper ferrite (B1Cu bulk= 4 MJ/m3) and cobalt ferrite (B1Co bulk= 55 MJ/m3). The results suggests that the source of magnetic anisotropy can be attributed to the coupling of the JT distortion with the magnetoelastic effect of Co. Instead of an indefinite increase with x, the magnetic anisotropy Ku tends to reach a saturation value due to the competition between the magnetoelastic effect of Co and the JT effect of Cu. Between the tetragonal x = 0.1 and the cubic x = 0.2 samples, the intrinsic magnetic anisotropy constant Ku values do not vary as significantly compared to the difference in the coercivity and the anisotropy fields. The reduction of anisotropy fields above x = 0.1 then can be attributed to the increase in the spontaneous magnetization.The coercivity analysis within the micromagnetic model revealed significant contribution to the coercivity by the microstructure and the local demagnetizing effect. The microstructure parameter αMM = 0.25 obtained was a classical value in the micromagnetic analysis, suggesting the departure of anisotropy field with this reduction factor. The effective local demagnetizing factor NeffMM of about 1.4 obtained were rather large suggesting a significant demagnetizing effect. Within the global model (GM) analysis, the values of NeffGM obtained were -0.38 for the x = 0.1 sample. The negative value suggests the presence of an exchange interaction acting effectively in opposition to the dipolar interaction. Below 100 K, discrepancy in the GM suggests the idea of a local heating event following the thermal activation due to the change in Zeeman energy and ineffective heat dissipation. This event may have led to the reduction of coercive field at sufficiently low temperature in the x = 0.1 sample assuming the grains are strongly exchange-coupled
Dondero, Russell A. "Silica coating of spinel ferrite nanoparticles." Thesis, Georgia Institute of Technology, 2000. http://hdl.handle.net/1853/27375.
Full textBrachwitz, Kerstin. "Defekt-induzierte Leitungsmechanismen und magnetische Eigenschaften spinellartiger Ferrite." Doctoral thesis, Universitätsbibliothek Leipzig, 2014. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-141251.
Full textAnderson, Richard M. "Magneto-optical properties of superparamagnetic spinel ferrite nanoparticles." Diss., Georgia Institute of Technology, 2002. http://hdl.handle.net/1853/30027.
Full textRondinone, Adam Justin. "Superparamagnetic relaxation dynamics of magnetic spinel ferrite nanoparticles." Diss., Georgia Institute of Technology, 2001. http://hdl.handle.net/1853/30958.
Full textVaughan, Lisa Ann. "Enviromentally benign synthesis and application of some spinel ferrite nanopartilces." Diss., Georgia Institute of Technology, 2011. http://hdl.handle.net/1853/44876.
Full textHeintz, Eva Liang-Huang. "Surface Biological Modification and Cellular Interactions of Magnetic Spinel Ferrite Nanoparticles." Diss., Georgia Institute of Technology, 2004. http://hdl.handle.net/1853/4944.
Full textCripps, Chala Ann. "Synthesis and characterization of cobalt ferrite spinel nanoparticles doped with erbium." Thesis, Georgia Institute of Technology, 2003. http://hdl.handle.net/1853/30855.
Full textLiu, Chao. "Correlation between superparamagnetic properties and chemical composition in some spinel ferrite nanoparticles." Diss., Georgia Institute of Technology, 2001. http://hdl.handle.net/1853/30391.
Full textSilva, Maya Dayana Penha da. "SÍNTESE E CARACTERIZAÇÃO DO SISTEMA ESPINÉLIOS CO1-XCUXFE2O4 (X = 1,0, 0,75,0,50, 0,25, 0,0) PELO MÉTODO DOS PRECURSORES POLIMÉRICOS." Universidade Federal do Maranhão, 2012. http://tedebc.ufma.br:8080/jspui/handle/tede/938.
Full textCoordenação de Aperfeiçoamento de Pessoal de Nível Superior
Ferrites are complex oxides, thermally stable, that presents crystalline structures equivalent to the spinel mineral.These solids alsoretain significant dielectric, magneticand catalytic properties. Thus, this work aims to obtain Co1-xCuxFe2O4spinel nanoparticles (x = 0.00, 0.25, 0.50, 0.75, 1.00) by the polymeric precursor method as well as evaluates the effect of its thermal treatment (700 - 1200 °C) over the crystalline structure. Therefore, all spinel structures were characterized by means of Raman and infrared vibrational spectroscopies and X-ray powder diffraction (XRPD). According to the X-ray diffraction patters, all the primary CoFe2O4 adopts an ideal inverse spinel structure [(Fd3 ̅m (O_h^7))], whereas the CuFe2O4 materials preferentially assume tetragonal distorted spinel structure [(I41/amd(D_4h^19))], except the 700 and 800 oC annealed CuFe2O4, that was indeed hematite. Besides, such case the FWHM analysis has indicates that the ternary thermal treatment leads to a higher organization of the lattice, as well as, increases the crystallite sizes. In general, the average crystallite sizes for CuFe2O4 varies between 27 35 nm; whereas, for the CoFe2O4 and Co-substituted CuF2O4 are respectively 28 37 nm and 33.3 52.6 nm. The crystal microdeformation oscillates between 0.17 and 0.32%, reducing, in most cases, with the thermal evolution. Raman spectra for CuFe2O4 samples shows vibrational modes at about 166 (F2g), 456 (F2g), 519 (F2g), 217 (Eg), e 686(A1g) cm-1. In other hand, CoFe2O4 samples present vibrational modes at 195, 457 and 587 cm-1 (all F2g symmetries), 298 cm-1 (A1g) and 671 cm-1(Eg). Similar optical-active modes were detected for the Co-substituted ferrites. Conversely, FTIR spectra for all CuFe2O4 shows characteristic stretching at about 531.79 559.45 cm-1 (Fe-O)A, 605.18 672.12 cm-1 (Cu-O)Aand 474.69 397.33 cm-1 (Fe-O)B. However, the CoFe2O4 samples exhibits strong stretching modes at 581.70 578.51 cm-1 (Co-O)A. Similar modes were also observed for the intermediary ferrites. Finally, the UV-vis spectra for CuFe2O4 shows 6A1g → 4Eg (G) (Fe3+ )B, and 6A1g → 4Eg (G) (Cu2+)Atransitions between 2.14 2.72 eV and 1.76 1.80 eV, respectively. However, the CoFe2O4 ferrites presents6A_1g → 2A_2g(P)(Co2+)A electronic transitions 2.11 and 2.39 eV.
As ferritas são óxidos compostos, termicamente estáveis, que apresentam estruturas cristalinas equivalentes as do mineral espinélio. Estas retêm propriedades dielétricas, magnéticas e catalíticas específicas. Neste sentido, este trabalho objetiva avaliar a síntese de estruturas espinélios Co1-xCuxFe2O4 (x = 1,0, 0,75, 0,25, 0,0) pelo método do precursores poliméricos (MPP), em diferentes temperaturas. Para tanto, tais sistemas foram caracterizados por difração de raios X (DRX) e espectroscópicas na região do infravermelho com transformada de Fourier (FTIR), Raman e UV-visível. Os resultados de DRX sugerem a formação de estruturas monofásicas CuFe2O4[(I41/amd(D_4h^19))] e CoFe2O4[(Fd3 ̅m (O_h^7))], a exceção das amostras CuFe2O4 700 e 800 oC.O parâmetro FWHM indica que o aumento da temperatura de calcinação ternária gera uma melhor organização estrutural a longo alcance. Ademias, o tamanho médio dos cristalitos aumenta com a temperatura de calcinação ternária devido a maior difusão dos íons na rede cristalina. Os tamanhos médios dos cristalitos variam entre 27 35 nm (CuFe2O4), 28 37 nm (CoFe2O4) e 33,3 - 52,6 nm(CuFe2O4 substituídas). As microdeformações da rede cristalina variaram entre 0,17 e 0,32%, diminuindo, na maioria dos casos, com a evolução da temperatura de tratamento. Os espectros Raman das amostras CuFe2O4exibem modos vibracionais próximos a 166 (F2g), 456 (F2g) , 519 (F2g), 217 (Eg), e 686(A1g) cm-1. Por outro lado, as estruturas CoFe2O4 demonstraram modos vibracionais F2g (195, 457 e 587 cm-1), A1g(298 cm-1) e Eg(671 cm-1). Modos vibracionais equivalentes foram também detectados nas estruturas intermediárias. Os espectros FTIR das CuFe2O4 exibiram estiramentos vibracionais nas regiões de 531,79 - 559,45 cm-1 (Fe-O)A, 605,18 - 672,12 cm-1(Cu-O)Ae 474,69 - 397,33 cm-1(Fe-O)B. Já as CoFe2O4 demonstraram uma forte absorção entre 581,70 - 578,51 cm-1(Co-O)A. Tais modos vibracionais também foram observados nas ferritas intermediarias. Os espectros UV-vis das CuFe2O4 exibiram transições 6A1g → 4Eg (G) (Fe3+ )B, entre 2,14 2,72 eV, e 6A1g → 4Eg (G) (Cu2+)A, entre 1,76 1,80 eV. Já as CoFe2O4 apresentam transições 6A_1g → 2A_2g(P)(Co2+)A entre 94, 2,11 e 2,39 eV.
Samia, Anna Cristina S. "Design and control of the superparamagnetic properties of cobalt-based spinel ferrite nanoparticles." Diss., Georgia Institute of Technology, 2002. http://hdl.handle.net/1853/31048.
Full textHaffer, Stefanie [Verfasser]. "Mesoporous spinel-type cobalt oxide, cobalt ferrite and alumina by nanocasting / Stefanie Haffer." Paderborn : Universitätsbibliothek, 2014. http://d-nb.info/1046651994/34.
Full textAssis, Raimison Bezerra de. "S?ntese e caracteriza??o de ferrita ni-zn pelo m?todo dos precursores polim?ricos calcinada por energia de microondas." Universidade Federal do Rio Grande do Norte, 2013. http://repositorio.ufrn.br:8080/jspui/handle/123456789/12816.
Full textCoordena??o de Aperfei?oamento de Pessoal de N?vel Superior
Magnetic ceramics have been widely investigated, especially with respect to intrinsic and extrinsic characteristics of these materials. Among the magnetic ceramic materials of technological interest, there are the ferrites. On the other hand, the thermal treatment of ceramic materials by microwave energy has offered various advantages such as: optimization of production processes, high heat control, low consumption of time and energy among others. In this work were synthesized powders of Ni-Zn ferrite with compositions Ni1- xZnxFe2O4 (0.25 ≤ x ≤ 0.75 mols) by the polymeric precursor route in two heat treatment conditions, conventional oven and microwave energy at 500, 650, 800 and 950?C and its structural, and morphological imaging. The materials were characterized by thermal analysis (TG/ DSC), X-ray diffraction (XRD), absorption spectroscopy in the infrared (FTIR), scanning electron microscopy (SEM), X-ray spectroscopy and energy dispersive (EDS) and vibrating sample magnetometry (VSM). The results of X-ray diffraction confirmed the formation of ferrite with spinel-type cubic structure. The extrinsic characteristics of the powders obtained by microwave calcination and influence significantly the magnetic behavior of ferrites, showing particles ferrimagn?ticas characterized as soft magnetic materials (soft), is of great technological interest. The results obtained led the potential application of microwave energy for calcining powders of Ni-Zn ferrite
Cer?micas magn?ticas t?m sido amplamente investigadas, principalmente com rela??o as caracter?sticas intr?nsecas e extr?nsecas destes materiais. Dentre os materiais cer?micos magn?ticos de interesse tecnol?gico, destacam-se as ferritas. Por outro lado, o tratamento t?rmico de materiais cer?micos por energia de microondas tem oferecido diversas vantagens, tais como: otimiza??o dos processos de obten??o, alto controle de aquecimento, menor consumo de tempo e energia entre outras. Neste trabalho, foram sintetizados p?s de ferritas Ni-Zn com composi??es Ni1-xZnxFe2O4 (0,25 ≤ x ≤ 0,75 mols) pela rota dos precursores polim?ricos em duas condi??es de tratamento t?rmico, em forno convencional e por energia de microondas a 500, 650, 800 e 950?C, e sua caracteriza??o estrutural, morfol?gica e magn?tica. Os materiais obtidos foram caracterizados por an?lises t?rmicas (TG/DSC), difra??o de raios x (DRX), espectroscopia de absor??o na regi?o do infravermelho (FTIR), microscopia eletr?nica de varredura (MEV), espectroscopia de raios X por dispers?o de energia (EDS) e magnetometria de amostra vibrante (VSM). Os resultados da difra??o de raios X confirmaram a forma??o da ferrita com estrutura c?bica do tipo espin?lio. As caracter?sticas extr?nsecas dos p?s obtidos e a calcina??o por microondas influenciaram de forma significativa o comportamento magn?tico das ferritas, apresentando part?culas ferrimagn?ticas, caracterizadas como materiais magn?ticos moles (macias), sendo de grande interesse tecnol?gico. Os resultados obtidos induziram o potencial de aplica??o de energia de microondas para a calcina??o de p?s de ferritas Ni-Zn
Sorrentino, Neto Antônio. "Síntese, caracterização e propriedades magnéticas de Ferritas de níquel – cobre." Universidade Federal da Paraíba, 2016. http://tede.biblioteca.ufpb.br:8080/handle/tede/9163.
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Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - CAPES
The ceramic oxides that exhibit ferromagnetic behavior are important commercial products for electronics industries and are commonly known as ferrites. In this work, we synthesized different compositions of CuxNi1-xFe2O4 ferrite with x = 0,0, 0,2, 0,4, 0,6, 0,8 and 1,0 by using the combustion method starting from the iron nitrate, nickel and copper and urea as a reducing agent. The powders were characterized by determination of specific surface area by the method (BET), X-ray diffraction (XRD), refinement of XRD data by the Rietveld method and vibrating sample magnetometry (MAV). The obtained copper nickel ferrites, referring x = 0,0, 0,2, 0,4, 0,6 synthesized had the same number of peaks corresponding to the single phase-forming powders that have been indexed to the spinel ferrite phase, forming a cubic phase and x = 0,8 to 1,0 tetragonal phase formed enhancing the efficiency of the applied method of synthesis. The refinement by the Rietveld method resulted in a determination of cell parameter of the samples, the cubic phase the value 0.8359 to 0.8340 nm and the crystallite size whose values occur between 239.62 to 187.24 nm. While in the tetragonal phase the cell parameter a = b was 5.8253 to 5,8230nm c = 8.5693 to 8.6941 nm. The hysteresis curves showed magnetic materials profile. The nickel ferrite - synthesized copper proved as materials with high potential for applicability in different areas of high-frequency devices such as phones and components for computers.
Os óxidos cerâmicos que exibem comportamento ferrimagnético representam importantes produtos comerciais para indústrias de eletrônica e são comumente conhecidos por ferritas. Neste trabalho, foram sintetizadas diferentes composições da ferrita CuxNi1-xFe2O4 com X = 0,0, 0,2, 0,4, 0,6, 0,8 e 1,0 pelo uso do método de combustão partindo-se dos nitratos de ferro, níquel e cobre e ureia como agente redutor. Os pós obtidos foram caracterizados por determinação de área superficial específica pelo método (BET), difração de raio X (DRX), refinamento dos dados de DRX pelo método Rietveld e magnetometria de amostra vibrante (MAV). As ferritas de níquel cobre obtidas, referentes x = 0,0, 0,2, 0,4, 0,6 sintetizadas apresentaram o mesmo conjunto de picos correspondentes à formação de pós monofásicos que foram indexados à fase espinélio de ferrita, formando uma fase cubica e para x = 0,8, 1,0 formou fase tetragonal predominante reforçando a eficiência do método de síntese aplicado. O refinamento pelo método de Rietveld resultou na determinação de parâmetro de cela das amostras, da fase cúbica o valor de 0,8359 a 0,8340 nm e do tamanho de cristalito cujos valores ocorrem entre 239,62 a 187,24 nm. Enquanto na fase tetragonal o parâmetro de cela a=b foi 5,8253 a 5,8230nm e c= 8,5693 a 8,6941 nm. As curvas de histerese mostraram perfil de materiais magnéticos. As ferritas de níquel - cobre sintetizadas se mostraram como materiais com alto potencial de aplicabilidade em diferentes áreas de equipamentos de alta frequência como telefonia e de componentes para de computadores.
Myndyk, Maxym, Mohammad Javad Nasr Isfahani, Dirk Menzel, Armin Feldhoff, Jamshid Amighian, Klaus-Dieter Becker, and Vladimír Šepelák. "Local structure and magnetic behavior of nanocrystalline MnZn spinel ferrite prepared by a one-step mechanochemical route." Universitätsbibliothek Leipzig, 2015. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-188008.
Full textMyndyk, Maxym, Mohammad Javad Nasr Isfahani, Dirk Menzel, Armin Feldhoff, Jamshid Amighian, Klaus-Dieter Becker, and Vladimír Šepelák. "Local structure and magnetic behavior of nanocrystalline MnZn spinel ferrite prepared by a one-step mechanochemical route." Diffusion fundamentals 12 (2010) 73, 2010. https://ul.qucosa.de/id/qucosa%3A13902.
Full textLüders, Ulrike Anne. "Development and integration of oxide spinel thin films into heterostructures for spintronics." Doctoral thesis, Universitat Autònoma de Barcelona, 2005. http://hdl.handle.net/10803/3373.
Full textHemos descubierto que el crecimiento epitaxial permite estabilizar fases nuevas del óxido NiFe2O4, fases que no existen en la forma másiva, y que tienen propiedades remarcablemente distintas. Como por ejemplo: un aumento dramático de la magnetización o la posibilidad de modificar drásticamente sus propiedades de transporte, pudiéndose obtener capas aislantes -como es en forma cerámica- o conductivas. Se ha realizado un estudio sistemático de los efectos del espesor de la capa y de las condiciones de crecimiento sobre las propiedades de magnetotransporte y los mecanismos de crecimiento.
Argumentamos que el aumento de la magnetización es debido a la estabilización de una fase NiFe2O4 espinela que es parcialmente inversa, en la que los iones Ni2+ están distribuidos entre las dos posiciones disponibles (tetraédrica y octaédrica) de la estructura. En la forma masiva del material los iones Ni solo se encuentran en los sitios octaédricos. La introducción adicional de vacantes de oxígeno es probablemente la causa de la existencia de una configuración electrónica mixta Fe2+/3+ en la subred octaédrica y de la alta conductividad de las capas.
Hemos aprovechado la capacidad de obtener epitaxias de NiFe2O4 ferrimagnéticas conductoras o aislantes para integrarlas en dos distintos dispositivos magnetoelectrónicos: una unión túnel magnética y un filtro de spin.
Las capas conductoras de NiFe2O4 se han empleado como electrodos ferrimagnéticos-metálicos en uniones túnel. El otro electrodo magnético es (La,Sr)MnO3 y la barrera túnel SrTiO3. Se ha podido medir una magnetoresistencia túnel importante hasta temperaturas tan altas como 280K. Los valores de magnetoresistencia corresponden a una polarización de spin del NiFe2O4 de aproximadamente un 40%, que es prácticamente independiente de la temperatura. Estos resultados sugieren que la nueva fase conductora que hemos estabilizado es un candidato interesante como fuente de corriente polarizada en spin.
Por otra parte, el NiFe2O4 aislante se ha implementado, por primera vez, como barrera túnel en una heteroestructura de filtro de spin. El electrodo magnético es (La,Sr)MnO3 y el electrodo no magnético Au. Hemos observado una magnetoresistencia túnel que alcanza valores de hasta un 50%. A partir de estas medidas, hemos deducido detalles relevantes de la estructura electrónica de la fase parcialmente inversa de NiFe2O4.
Hemos crecido el óxido CoCr2O4 sobre distintos substratos, tales como MgO(001) y MgAl2O4(001). Hemos podido comprobar que este óxido presenta una pronunciada tendencia a un crecimiento 3D. Por esta razón, las superficies de la capa no son nunca suficientemente planas y no se pueden usar en heteroestructuras túnel.
Sin embargo hemos aprovechado esta característica para controlar el crecimiento de estas estructuras 3D y hemos conseguido la formación de objetos submicrónicos, autoorganizados con formas piramidales muy bien definidas. El estudio detallado del efecto de los parámetros de crecimiento nos ha permitido por una parte, dilucidar cuales son los mecanismos que llevan a una autoorganización tan perfecta y por otra determinar que, en las condiciones adecuadas, se pueden obtener templates totalmente faceteados con múltiples posibilidades para futuras aplicaciones.
In this thesis the growth of thin films of NiFe2O4 and CoCr2O4 by RF sputtering on different oxide substrates and the characterization of their magnetic and electric properties is reported. The aim is to integrate the films into spintronic devices namely magnetic tunnel junctions and spin filter.
It was found that the epitaxial growth of these films permits to stabilize new phases of NiFe2O4, which are not found for the bulk material and which show remarkably distinct properties. A strong enhancement of the saturation magnetization was found as well as the possibility to tune the electric behaviour of the films from insulating - like in bulk NiFe2O4 - to conducting. A systematic study of the influence of the film thickness and growth parameters on the properties of the films was carried out.
The enhancement of the saturation magnetization can be explained by a partially inversed spinel structure, where the Ni2+ ions are distributed over both available sites (octahedral and tetrahedral) of the structure, whereas in bulk NiFe2O4 the Ni2+ ions are only located on the octahedral sites of the structure. An additional introduction of oxygen vacancies causes the formation of mixed valence Fe2+/3+ chains on the octahedral sites and thus a hopping conductivity.
We have taken advantage of our ability to obtain epitaxial ferromagnetic NiFe2O4 films of insulating or conducting character to integrate them in two different spintronic devices: the magnetic tunnel junction and the spin filter.
The conducting NiFe2O4 was integrated in a magnetic tunnel junction as a magnetic electrode, with a (La,Sr)MnO3 counterelectrode and a SrTiO3 barrier. A magnetoresistance was measured up to a temperature of 280K. The values of the magnetoresistance correspond to a spin-polarization of 40%, which is basically constant in temperature. This results show that the conductive phase of NiFe2O4 is an interesting candidate for the application as a source of highly spin-polarized current.
On the other hand the insulating NiFe2O4 has been integrated into a spin filter as the magnetic barrier. The magnetic electrode was again (La,Sr)MnO3 and the counter electrode Au. A magnetoresistance up to 50% was observed. It was possible to deduce the band structure of NiFe2O4 from these measurements.
Thin films of CoCr2O4 were grown on different substrates like MgO(001) or MgAl2O4(001). It was found that the material shows a pronounced tendency to grow in a three dimensional manner. Thus the surface of these films is not sufficiently smooth to integrate them into tunnel contacts.
However, we were able to control the growth and morphology of the three dimensional structures leading to the formation of submicron self-organized pyramids with a square or elongated base. By a detailed study of the influence of the growth parameters it was possible to elucidate the underlying growth mechanisms and to obtain a fully faceted surface, which can be used in different applications.
Rodrigues, ?dila Priscilla Gomes. "S?ntese e caracteriza??o de ferritas de n?quel dopadas com cobalto e efeito da substitui??o nas suas propriedades magn?ticas." Universidade Federal do Rio Grande do Norte, 2014. http://repositorio.ufrn.br:8080/jspui/handle/123456789/17766.
Full textCoordena??o de Aperfei?oamento de Pessoal de N?vel Superior
The ferrite composition Ni1 - xCoxFe2O4 (0 ≤ x ≤ 0.75) were obtained by the method of microwave assisted synthesis and had their structural and magnetic properties evaluated due to the effect of the substitution of Ni by Co. The compounds were prepared: according to the concept of chemical propellants and heated in the microwave oven with power 7000kw. The synthesized material was characterized by absorption spectroscopy in the infrared (FTIR), Xray diffraction (XRD) using the Rietveld refinement, specific surface area (BET) , scanning electron microscopy (SEM) with aid of energy dispersive analysis (EDS) and magnetic measurements (MAV). The results obtained from these techniques confirmed the feasibility of the method of synthesis employed to obtain the desired spinel structure, the ferrite, nickel ferrite as for nickel doped with cobalt. The results from XRD refinement ally showed the formation of secondary phases concerning stages α - Fe2O3, FeO, (FeCo)O e Ni0. On the other hand, there is an increase in crystallite size with the increase of cobalt in systems, resulting in an increased crystallinity. The results showed that the BET systems showed a reduction in specific surface area with the increase of cobalt and from the SEM, the formation of irregular porous blocks and that the concentration of cobalt decreased the agglomerative state of the system. The magnetic ferrites studied showed different characteristics according to the amount of dopant used, ranging from a very soft magnetic material (easy magnetization and demagnetization ) - for the system without cobalt - a magnetic material with a little stiffer behavior - for systems containing cobalt. The values of the coercive field increased with the increasing growth of cobalt, and the values of saturation magnetization and remanence increased up to x = 0,25 and then reduced. The different magnetic characteristics presented by the systems according to the amount of dopant used, allows the use of these materials as intermediates magnetic
As ferritas de composi??o Ni1−xCoxFe2O4 (0≤x≤0,75) foram obtidas atrav?s do m?todo de s?ntese assistida por microondas e tiveram suas propriedades estruturais e magn?ticas avaliadas em fun??o do efeito da substitui??o do Ni pelo Co. Os compostos foram preparados de acordo com o conceito da qu?mica dos propelentes e aquecidos em forno micro-ondas com pot?ncia 7000kw. O material sintetizado foi caracterizado por espectroscopia de absor??o na regi?o do infravermelho (FTIR), difra??o de raios X (DRX), com o uso do refinamento pelo m?todo de Rietveld, ?rea superficial espec?fica (BET), microscopia eletr?nica de varredura (MEV) com aux?lio de an?lise por dispers?o de energia (EDS) e medidas magn?ticas (MAV). Os resultados obtidos, a partir destas t?cnicas confirmaram a viabilidade do m?todo de s?ntese empregado para a obten??o da estrutura espin?lio desejada, tanto para a ferrita de n?quel quanto para as ferritas de n?quel dopadas com cobalto. Os resultados do DRX, aliado ao refinamento, mostraram a forma??o de fases secund?rias tais como as fases α - Fe2O3, FeO, (FeCo)O e Ni0. Por outro lado, observou-se um aumento no tamanho do cristalito com o incremento do cobalto nos sistemas, implicando em um aumento da cristalinidade. Os resultados do BET mostraram que os sistemas apresentaram uma redu??o da ?rea superficial espec?fica com o incremento do cobalto e a partir do MEV observou-se a forma??o de blocos porosos irregulares e que o aumento da concentra??o de cobalto dimunuiu o estado de aglomera??o dos sistemas. As ferritas estudadas apresentaram caracter?sticas magn?ticas diferenciadas de acordo com a quantidade do dopante utilizado, variando de um material magn?tico bastante mole (f?cil magnetiza??o e desmagnetiza??o) - para o sistema sem cobalto - a um material magn?tico com comportamento um pouco mais duro - para os sistemas contendo cobalto. Os valores do campo coercitivo aumentaram com o crescente incremento do cobalto, e os valores de magnetiza??o de satura??o e reman?ncia aumentaram at? x=0,25 e depois reduziram. As caracter?sticas magn?ticas diferenciadas apresentadas pelos sistemas, de acordo com a quantidade de dopante utilizado, permite o uso desses materiais como magn?ticos intermedi?rios
Silva, Jos? Eves Mendes da. "S?ntese, caracteriza??o de ferritas espin?lio com propriedades magn?ticas e absorvedoras de microondas." Universidade Federal do Rio Grande do Norte, 2013. http://repositorio.ufrn.br:8080/jspui/handle/123456789/17768.
Full textCoordena??o de Aperfei?oamento de Pessoal de N?vel Superior
Were synthesized spinel-type ferrites with general formula Ni0,8Mg0.2-xMxFe2O4, where M represents the doping Mn, Co or Mn + Co simultaneously, x ranges for the values 0.02, 0.05 and 0.1. The value of x was divided by 2 in cases where M equals Mn and Co conjugates. We used the citrate precursor method and heat treatment to obtain the phases at 1100?C. The materials were characterized by XRD, TGA/ DTGA, SEM, MAV and reflectivity measurements by the method of waveguide. Powders to 350?C/3.5 h were crystalline and nanosized. According to the results this temperature all powders have a percentage of ferrite phase over 90%. The composition had the addition of Mn and Co simultaneously showed a higher percentage of secondary phase NiO, 5.8%. The TGA/DTGA curves indicate that this sample reached phase (s) crystalline (s) at lowest temperatures. The X-ray diffractograms of the samples calcined at 350?C and 1100?C were treated with the Rietveld refinament technique. The powders calcined at 1100 ?C/3h in air show to be 100% except spinel phase composition with 0.02 doping. The micrographs show clusters of particles with sizes smaller than 1 μm in calcination temperature of 1100?C which agreed with the result of Rietveld refinement. In the compositions doped with Mn were higher values of magnetization (45.90 and 53.20 Am2/kg), which did not cause high microwave absorption. The theoretical calculation of magnetization (MT) was consistent with the results, considering that there was agreement between the increase of magnetization experimental and theoretical. It was observed that there was the interrelation of the final effect of absorption with the thickness of MARE, the composition of ferrimagnetic materials and in particular the specific values of frequency. The analysis shows that the reflectivity increases in the concentration of cobalt increased the frequency range and also for absorption 10.17 GHz and 84%, respectively. The best result of chemical homogeneity and the value of 2.96 x 10-2 tesla coercive field were crucial for high performance ferrite absorber with 0.1 cobalt. The Cobalt has high magnetocrystalline anisotropy, it is associated with an increased coercive field, Hc. Therefore, this property improves the results of reflectivity of spinel ferrites
Foram sintetizadas ferritas do tipo espin?lio com f?rmula geral Ni0,8Mg0,2-xMxFe2O4, onde M representa os dopantes Mn, Co ou Mn + Co simultaneamente, x varia para os valores 0,02; 0,05 e 0,1. O valor de x foi dividido por 2 nos casos em que M equivale a Mn com Co conjugados. Foi utilizado o m?todo dos citratos precursores e tratamento t?rmico na obten??o das fases a 1100?C. Os materiais foram caracterizados por DRX, TGA/DTGA, MEV, MAV e medidas de refletividade pelo m?todo de guia de ondas. Os p?s a 350?C/3,5h foram cristalinos e nanom?tricos. De acordo com os resultados nesta temperatura todos os p?s apresentam um percentual de fase ferrita superior a 90%. A composi??o que teve a adi??o de Mn e Co simultaneamente apresentou maior percentual de fase secund?ria NiO, 5,8%. As curvas TGA/DTGA indicam que essa amostra alcan?ou fase(s) cristalina(s) em temperaturas mais baixas. Os difratogramas de raios X das amostras calcinadas a 350?C e 1100?C foram tratados pela t?cnica de refinamento Rietveld. Os p?s calcinados a 1100?C/3h em atmosfera ambiente mostram ser 100% de fase espin?lio exceto a composi??o com 0,02 de dopantes. As micrografias apresentam aglomerados de part?culas com tamanhos menores que 1 μm na temperatura de calcina??o de 1100?C, o que concordou com o resultado de refinamento Rietveld. Nas composi??es dopadas com Mn ocorreram os maiores valores de magnetiza??o (45,90 e 53,20 Am2/kg), o que n?o acarretou alta absor??o de microondas. O c?lculo te?rico da magnetiza??o (MT) foi coerente com os resultados, considerando-se que houve concord?ncia entre o aumento das magnetiza??es experimental e te?rica. Observa-se que houve interrela??o do efeito final de absor??o com a espessura do MARE, a composi??o do material ferrimagn?tico em particular e os valores espec?ficos de freq??ncia. A an?lise de refletividade indica que o aumento na concentra??o de cobalto aumentou a faixa de freq??ncia e a absor??o para 10,17 GHz e 84%, respectivamente. O resultado indica que a melhor homogeneidade qu?mica e o valor 2,96 x 10-2 tesla de campo coercitivo foram determinantes para o alto desempenho absorvedor da ferrita com 0,1 de cobalto. O Cobalto tem alta anisotropia magnetocristalina, isto est? associado ao aumento do campo coercitivo, Hc. Portanto, essa propriedade melhora os resultados de refletividade das ferritas espin?lio
Abbali, Zineb. "Etude de la cristallisation de ferrites spinelles dans des verres borates." Grenoble 2 : ANRT, 1988. http://catalogue.bnf.fr/ark:/12148/cb376110731.
Full textTailhades, Philippe. "Elaboration, caracterisation et optimisation des proprietes morphologiques et magnetiques de ferrites lacunaires destines a l'enregistrement haute densite." Toulouse 3, 1988. http://www.theses.fr/1988TOU30185.
Full textEL, HARFAOUI MOHAMMED. "Etude de l'etat magnetique localement cante et de sa dynamique dans le ferrite de lithium-titane dilue." Paris 6, 1988. http://www.theses.fr/1988PA066650.
Full textBui, Thi Mai Anh. "Etude de la décomposition spinodale de cobaltite de fer sur couches minces." Thesis, Toulouse 3, 2015. http://www.theses.fr/2015TOU30028/document.
Full textThis work aimed to study the effects of spinodal decomposition process on structural and microstructural evolution of cobaltite thin films whose composition is in the miscibility gap of CoFe2O4 - Co3O4 system. At the first time, thin films were elaborated by RF magnetron sputtering from a ceramic target with average composition of Co1.73Fe1.27O4. Deposits at high argon pressure or high RF power favor the formation of thin films containing an oxide phase associated with a spinel phase. The oxide phase obtained in these films is probably in part due to the reduction of the target surface owing to a strong bombardment, without excluding the presence of a physical phenomenon related to the thermalization of oxygen atoms. Deposition conditions were optimized at 0.5 Pa - 20 W. That allows a compromise between a small amount of oxide phase in the thin films and an acceptable deposition rate. Spinodal decomposition has been demonstrated on the thin films deposited in this condition and post-annealed at 600 ° C for various times. The characterizations by X-ray diffraction, Raman spectroscopy and VSM magnetic measurements, have confirmed the gradual formation of a two-phase system made of a cobalt-rich phase and an iron-rich phase. However, the formation of periodic zones, corresponding to these two phases, was not observed on the decomposed thin films. These two phases exhibit in fact a very small difference in their structure. Finally, the studies on thin films annealed at lower temperatures (for example at 450 ° C) showed evolutions similar to those observed during treatment at 600 ° C. Spinodal transformation seems to be initiated by a migration of divalent cations into the tetrahedral sites and trivalent cations into octahedral sites. The spinel structure thus tends to turn into a normal structure, before the separation into two spinel phases, due to the spinodal transformation
Ammar, Mehdi. "Étude du magnétisme de composites métal-oxyde et métal-diélectrique nanostructurés pour composants passifs intégrés." Phd thesis, École normale supérieure de Cachan - ENS Cachan, 2007. http://tel.archives-ouvertes.fr/tel-00371362.
Full textHolec, Petr. "Magnetické nanočástice a nanokompozitní materiály se spinelovou strukturou, jejich příprava a charakterizace." Doctoral thesis, 2012. http://www.nusl.cz/ntk/nusl-326583.
Full textZviagin, Vitaly. "Ellipsometric Determination of Cation Disorder in Magnetically Ordered Spinel Ferrite Thin Films." 2019. https://ul.qucosa.de/id/qucosa%3A35443.
Full text江偉菁. "Study on the magnetic properties of spinel ferrites MFe2O4 (M=Mn, Fe, Co, Ni, Zn and Mg) nanoparticles." Thesis, 2006. http://ndltd.ncl.edu.tw/handle/83098216779658062033.
Full text國立彰化師範大學
物理學系
94
The magnetic properties of ferrites with spinel structure have been researched widely at 1950’s, but most research was carried out for bulk samples. In resent years, nanoparticles of ferrites have attracted a lot of attention because of the need of magnetic recording material. In this thesis, we have investigated the magnetic properties of MFe2O4 nanoparticles with different doping metals which was prepared by sol-gel method, where M = Mn、Fe、Co、Ni、Zn、Mg. The structure and particle size were determined by X-ray powder diffractometer. Magnetic properties were measured by electron spin resonance spectrometer ( ESR ) , superconducting quantum interference device ( SQUID ) , and alternating gradient magnetometer ( AGM ) . We find that different preparing condition can change the magnetic properties of samples. For example, the saturated magnetization of MnFe2O4 prepared in a pH = 3 solution is 3.16 times that prepared in a pH = 5 solution at 6 K. As to size effect, the nanoparticles show different characteristics from bulk samples on both the rate of change with temperature and the magnitude of magnetic properties. In the samples we studied, the magnetic-doping-metal sample has stronger magnetic nature, while the nonmagnetic-doping-metal sample shows paramagnetic-like behavior at high temperature. The cation distribution in ferrites influence the magnetic properties of ferrites obviously.
Brachwitz, Kerstin. "Defekt-induzierte Leitungsmechanismen und magnetische Eigenschaften spinellartiger Ferrite." Doctoral thesis, 2013. https://ul.qucosa.de/id/qucosa%3A12425.
Full textHsieh, Chang-Tsun, and 謝長村. "Domain Wall and Spin Resonance Studies of Spinel Ferrite Nanoparticles and Nickel thin films." Thesis, 2003. http://ndltd.ncl.edu.tw/handle/12020619175987222020.
Full text國立清華大學
物理學系
92
Domain wall and spin resonance of magnetic thin films and nanoparticles are investigated in this dissertation. Two main thrusts are: (1) electron spin resonance studies of quantum phase transition in magnetic nanoparticles, and (2) magnetic force microscopic studies of domain walls on thin nickel films. Sol-gel glass embedded with iron nanoparticles provides fascinating features inheriting with paramagnetic, ferromagnetic, and superparamagnetic resonance properties under various compositional weight ratios and annealing conditions. Two spectra arising from paramagnetic Fe3+ ions and ferrimagnetic Fe2O3 particles both centered at ge =2.0 compete with intensities as the annealing temperature TA increases. The asymmetric and rather broad line shape can be elucidated by the ferromagnetic resonance of the single domain Fe2O3 nanoparticles. The half linewidth simulation agrees well with the super paramagnetic resonance theory of particle size ~10.5 nm. The classical, thermally driven transition from ferrimagnets to superparamagnets in Fe3O4 nanoparticles can be converted into another quantum phase by a strong internal anisotropic field. The field induced by crystal anisotropy, which is perpendicular to the Ising axis can destroy the magnetic long-range order to quantum paramagnets by exceeding some critical values. Electron spin resonance (ESR) spectrometer, a very sensitive instrument with fast detecting window to explore quantum phase transition for magnetic nanoparticles, was exploited to study the fascinating interplay between thermal and quantum fluctuation in the vicinity of a quantum critical point. We have determined the static spin susceptibility and critical exponent g, which is power-law dependent spanning the quantum critical point and investigated the effects of various microwave fields, particle sizes, and temperature dependence on the magnetic states of single domain spinel ferrite nanoparticles. As temperature decreases, the spectrum behaves from superparamagnetic (SPR) to ferromagnetic resonance (FMR) and retrieves to quantum superparamagnetic as the temperature lowers down further. On account of the highly anisotropy field of Co-ferrite, the quantum critical behavior of CoFe2O4 nanoparticles is prominently observed. We have combined magnetization measurement and electron spin resonance to study the fascinating quantum tunneling of magnetization in Co-ferrite nanoparticles at low temperatures. ESR spectra are shifted to low fields (1600G) at 35 K accompanying with the intensity increasing and linewidth narrowing. The increasing of magnetic moment at low-temperature (below 11 K) and the extraordinarily small coercive field (1.3 kOe) at 2K of Co-ferrite NPs are investigated by magnetization measurements. A new approach, Heisenberg model with strong easy-plane anisotropy, is proposed to attribute these to the conversion of ferrimagnets to quantum superparamagnets (short-range ordered). The quantum superparamagnetic size is estimated about~1.5nm corresponding to the short-range ferromagnetically correlated volumes existing in MNPs. Magnetic force microscopy images with a resolution as high as 3 nm are examined for thin nickel films deposited by argon ion sputtering method. Samples grown at 100∘C with grain sizes of near 60nm exhibits coexistence of Bloch and Neel walls whereas samples grown at room temperature with grain size of ~10nm display an alternative Bloch line with a cap switch. The relationship between domain size and film thickness follows a law (where d is the film thickness) as predicted by Kittel.
FitriWidhiastuti and 魏巧玲. "Remediation of boron from aqueous solution by electrochemically co-precipitated spinel ferrite in electrocoagulation process." Thesis, 2017. http://ndltd.ncl.edu.tw/handle/2tk447.
Full text國立成功大學
化學工程學系
105
Electrocoagulation process using transition metals as electrolytes and sacrificial anodes was studied for the removal of boron through formation spinel ferrites. The spinel ferrite (MFe2O4, M = Fe, Cu, Ni, and Co) evolved during electrocoagulation could be promising adsorbents for boron. The parameters such as pH (4 – 12), current density (1.25 – 5 mA/cm2), boron initial concentration (10 – 100 mg/l), and combination pairs of electrodes were studied. The efficiency of boron removal could achieve 95% as electrocoagulation was optimized at conditions: initial B = 10 mg/l, reaction pH 8 ± 0.5, current density = 3.75 mA/cm2, and 60 min reaction. X-ray diffraction (XRD) patterns revealed that several spinel type such as nickel ferrites, cobalt ferrites and copper ferrites were obtained by electrocoagulation process. The adsorption isotherms of spinel type materials fitted by Langmuir and Freundlich models indicated that qmax of nickel ferrites was 28.90 mg/g with pHpzc 10.25. Most of the spinel ferrites were granular crystallites with the crystalline size of around 26 – 30 nm. The highest saturation magnetization was nickel ferrites 50.30 emu/g by vibrating sample magnetometer (VSM) analysis. Magnetic separable spinel ferrites offers easier solid - liquid separation after electrocoagulation process.
Ou, Jeng-Lung, and 歐政隴. "The study of microwave absorbing properties for composites β-SiC/spinel Mn-Zn ferrite/carbon black." Thesis, 2011. http://ndltd.ncl.edu.tw/handle/30673496864709810958.
Full text國防大學中正理工學院
應用化學碩士班
99
Nano MnZn cubic ferrite powders (Mn1-XZnXFe2O4) were prepared by sol-gel aqueous combustion synthesis (ACS) method in this study. The starting materials of Fe, Mn, and Zn nitrates were used as the sources of metallic ions and oxidizing agents, while glycine was applied as the reducing agent as well as the chelating reagent. Accordingly, the metallic nitrates combined with glycine in aqueous solution forming complex ions. Spinel structure of the final product was driven by the self-propagation combustion of the sol-gel solution. X-ray diffraction pattern of the as-burnt product indicated a cubic or spinel ferrites crystal structure. Scanning electron microscopy (SEM) images revealed that the grain sized of the as-burnt powders ranged in 60~100 nm. However, the average diameter of the powder after a heat treatment at 1200 ℃ were found at ~1.0 μm. For a composition of Mn0.8Zn0.2Fe2O4, the powders were obtained to have the optimal magnetic properties by using VSM instrument. The saturated magnetization (Ms), remanence magnetization (Mr), and the coercivity (Hc) of Mn0.8Zn0.2Fe2O4 are 109.80 emu/g, 11.712 emu/g and 81.398 Oe, respectively. Because of the only magnetic lose properties of the Mn-Zn spinel ferrites can have, therefore the conductive carbon black and dielectric material of β-SiC were mixted with ferrites and organic polymers to form the high absorbability and low density of microwave absorbing composite materials. In which Agilent Technologies E8362B Analyzer were used to characterize the microwave absorption properties of the materials.
"Synthesis and Characterization of Nanocrystalline Nickel-Zinc Spinel Ferrite Thin Films Using the Spin-Spray Deposition Method." Doctoral diss., 2013. http://hdl.handle.net/2286/R.I.17906.
Full textDissertation/Thesis
Ph.D. Materials Science and Engineering 2013
Hsu, Wei-mau, and 徐維懋. "Materials Characteristics of Spinel Nickel Ferrite Oxygen Carrier and It’s Selection of Inert Supports for Chemical Looping Combustion Process." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/01088156383690048443.
Full text國立臺灣科技大學
機械工程系
100
Chemical looping combustion (CLC) process is a promising technology of CO2 capture and sequestration (CCS) with high energy efficiency and low emission of greenhouse gases. For the practical use, the performance of oxygen carriers is a key issue for the application on CLC process. Unfortunately, the formation of inactive compounds by the interaction between the ordinary metal oxygen carriers and inner supported were evidently encountered in a CLC process, which subsequently reduced the performance of CLC process. In our preliminary results, after 5 successive cycles, NiFe2O4 powder with a single phase of spinel structure represented a higher redox cycling behavior and stability as compared to the standard of NiO and Fe2O3. To identify the initial reduction mechanism of NiFe2O4, we obtained the activation energy (Ea) of the reduction behavior using the reduction rate equation and Arrhenius equation. However, at long redox cycles (10 cycles), the performance of NiFe2O4 oxygen carriers was dramatically reduced due to the agglomeration of oxygen carriers. Thus, the addition of inner materials as the supports to oxygen carriers is a necessary process to prepare a superior oxygen carrier system in the operation of long redox cycles in CLC process. This study is to investigate the effects various inner supports (Al2O3, ZrO2 and YSZ) of in NiFe2O4 oxygen carrier system and the performance of CLC process by TGA system. Mingled various inner supports shift the reduction kinetics of oxygen carriers, NiFe2O4/Al2O3 system decayed the reduction kinetics but both NiFe2O4/ZrO2 and NiFe2O4/YSZ system promoted the reduction kinetics. To identify the initial reduction mechanism and activation energy, NiFe2O4/Al2O3 system’s activation energy is 83.4 kJ/mol reduction mechanism controlled by solid-state diffusion. For the systems of NiFe2O4/ZrO2 and NiFe2O4/YSZ, both reduction mechanisms are mainly dominated by gas diffusion with the activation energy values of 9.0 kJ/mol and 10.1 kJ/mol, respectively. Our results also demonstrated the higher redox cycling behavior of using the proposed preparation of NiFe2O4 as an oxygen carrier with Al2O3 support in a reversible chemical looping process (CLP).
Hsu, Chia-Shuo, and 許家碩. "Systematic investigation of spinel-type ferrite MFe2O4 (M = Mn, Fe, Co, Ni, Zn): in-situ and ex-situ X-ray approaches to oxygen evolution reaction." Thesis, 2016. http://ndltd.ncl.edu.tw/handle/11900529667026818271.
Full text國立臺灣大學
化學研究所
104
Metal oxide of spinel family has performed great potential to replace RuO2 or IrO2 toward oxygen evolution reaction (OER), but the fundamental mechanism of spinel oxides is still far from a complete understanding especially for the role of metal ions. Owing to various coordinated sites of divalent/trivalent metals ions and surface condition (mor-phology and defects), it’s a great challenge to have a fair assessment of electrocatalytic performance of spinel system. Herein, we demonstrated a series of MFe2O4 (M = Mn, Fe, Co, Ni, Zn) family with a well-controlled morphology to achieve comprehensive study of electrocatalytic activity toward OER, in which most of the divalent metals (M2+) of MFe2O4 were located at octahedral sites and well-defined single-crystal nanocubes were synthesized to minimize the influence caused by crystallographic sites/morphology of variables for each samples. The effects of M2+ ion in MFe2O4 can be realized through investigating the OER behaviors of MFe2O4 and that of γ-Fe2O3 as a reference to have in-depth understanding of the roles of divalent/trivalent metal ions. In-situ X-ray diffraction and ex-situ X-ray absorption spec-troscopies were employed to provide direct evidence that the superior OER activities of CoFe2O4 and NiFe2O4 samples could be attributed to a remarkable phase transformation forward metal oxyhydroxide, while the rest of compounds remain unchanged during oxygen evolution reaction.