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microstructure and magnetic state of fe o sio colloidal

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  • Microstructure of implanted Fe nanoparticles in silica

    O 3) are shown. Depending on the Fe oxidation state the XANES spectra vary systematically in the position of the pre-edge peaks (7.11 7.12keV). The peak position shifts to low energies with decreasing the valence number of Fe ion. From this result pre-edge peaks for the Fe implanted samples help us estimate Fe oxidation state in SiO 2. Aug 28 2019 · Formation of SiO 2-SiO 2 Composite Particles with Size Control. In this investigation in order to demonstrate the feasibility of designing a composite that consists of the same material but of different sizes SiO 2 with particle sizes of 1 4 and 16 μm (Ube EXYMO) were used. As for the primary 16-μm SiO 2 particles an LbL coating of PDDA/PSS/PDDA/PSS was carried out while as for the

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  • Micro- and Nano-assembly of Composite Particles by

    Aug 28 2019 · Formation of SiO 2-SiO 2 Composite Particles with Size Control. In this investigation in order to demonstrate the feasibility of designing a composite that consists of the same material but of different sizes SiO 2 with particle sizes of 1 4 and 16 μm (Ube EXYMO) were used. As for the primary 16-μm SiO 2 particles an LbL coating of PDDA/PSS/PDDA/PSS was carried out while as for the O 3) are shown. Depending on the Fe oxidation state the XANES spectra vary systematically in the position of the pre-edge peaks (7.11 7.12keV). The peak position shifts to low energies with decreasing the valence number of Fe ion. From this result pre-edge peaks for the Fe implanted samples help us estimate Fe oxidation state in SiO 2.

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  • Structure and magnetic properties of SiO2-coated Co

    K in a magnetic field of 5.5 T. As shown in Fig. 4 the loop for the nanoparticles calcined at 900°C is symmetrical about zero field and the exchange bias fieldHex is just about 3.9 Oe which is quite smaller than the coercivity field.

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  • SOL-GEL Fe NANOCOMPOSITES

    9 540 ν Si-O-Si from cyclic tetramers 1–3 10 530 ν Fe-O 2 11 461 δ Si-O-Si 1–3 3.2. XRD RESULTS The XRD results have shown in all cases besides the broad band characteristic for the presence of the amorphous silica gel the nanometric crystallization of α-Fe2O3. The degree of crystallization depends on the type of matrix and the −222 − Microstructure and Magnetic State of Fe3O4-SiO2 Colloidal Particles−P. V. Kharitonskii et al. 16 17 where the Larmor frequency f0 is of the order of 109 s−1. Because the particle volume V and temperature T are both in the exponent the value of τ is strongly

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  • High coercivity SmCo 5 synthesized with assistance of

    Feb 25 2021 · The APS of SmCo 5 particles can be tuned from 740 to 504 nm by controlling the volume of the added colloidal SiO 2 suspension. As-prepared Microstructure and Magnetic Properties of Aerosol-Deposited Sm-Fe-N Thick Films TOMOHITO MAKI 1 SATOSHI SUGIMOTO 1 TOSHIO KAGOTANI 1 KOICHIRO INOMATA 1 and JUN AKEDO 2 1Tohoku University Japan 2National Institute of Advanced Industrial Science and Technology Japan SUMMARY In this study the relationship among magnetic prop-

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  • Synthesis and detection the oxidization of Co cores of Co

    Up to now there are many magnetic core-shell materials which have been made including Fe 2 O 3 SiO 2 /Ag Fe 3 O 4 SiO 2 Fe 3 O 4 SnO 2 Co SiO 2 Pt CoO FePt SiO 2 Fe 3 O 4 Au Fe 2 O 3-CdSe SiO 2 and Fe 3 O 4 /γ-Fe 2 O 3 SiO 2 15-23 . For example the Fe 3 O 4 SiO 2 is a common magnetic core-shell nanoparticle. The core particle in the ferromagnetic state. The saturation magnetization was measured to be 9.17 kGs at 5 K and 9.07 kGs at 300 K which is in good agreement with the expected values. It is known that the hysteresis loop of the Co/CoO or Co/Co3O4 system will be displaced along the field axis if the system is cooled in a magnetic field due to ferromagnetic–

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  • Magnetochromatic Microspheres Rotating Photonic Crystals

    Fe 3 O 4 SiO 2 core/shell colloids were then prepared through a modified Stöber process. The magnetic colloids and photoinitiator DMPA (5 wt ) were dispersed in PEGDA-700 to form a brown homogeneous solution with a Fe 3 O 4 concentration of 8 mg/mL. In a typical process 1.5 mL of PEGDA precursor solution were mixed with 21 mL of mineral oil The effect of weak quasistatic magnetic field (QSMF) the strength of which is of the order of 100 A/m can be detected using colloidal solutions of Fe m O n -SiO 2 NPs by changing the electrical

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  • Correlating dynamic microstructure to observed color in

    Jul 27 2020 · Representative images of the observed structural color response as a function of voltage for each concentration of Fe 2 O 3 / SiO 2 particles. After applying 5 V the field was removed (OFF) and the color was observed to approach its initial state. The scale bar is 5 mm. Reuse Permissions Microstructure and Magnetic Properties of Aerosol-Deposited Sm-Fe-N Thick Films TOMOHITO MAKI 1 SATOSHI SUGIMOTO 1 TOSHIO KAGOTANI 1 KOICHIRO INOMATA 1 and JUN AKEDO 2 1Tohoku University Japan 2National Institute of Advanced Industrial Science and Technology Japan SUMMARY In this study the relationship among magnetic prop-

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  • Improved Photocatalytic Performance of a Novel Fe3O4 SiO2

    The composition and structure of the products were also measured by infrared (IR) spectra. As shown in Figure 3 the typical Fe-O stretching bands at 584 cm −1 can be found in all samples indicating existence of magnetic core in composites. The Fe 3 O 4 SiO 2 sample showed the bending symmetric and asymmetric stretching vibration of Si-O-Si at 482 cm −1 790 cm −1 and 1083 cm −1 Replacing the SiO2 support with magnetic Fe3O4 the obtained hybrid Au/Fe 3 O 4 NPs have been considered as promising candidates for in-vivo diagnostic tests that include both optical detection and targeting capabilities under an external magnetic field. 18 19 Using Rh

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  • Solid State Phenomena Vol. 247 p. 3 Scientific

    The Investigation of Superparamagnetic Colloidal Particles Fe m O n-SiO 2 Authors Peter V. Kharitonskii Kamil G. Gareev A.M. Frolov S.V. Lebedev P.V. Velikorussov Abstract Colloidal particles based on iron oxides and silica were obtained by sol-gel method. Jul 27 2020 · Representative images of the observed structural color response as a function of voltage for each concentration of Fe 2 O 3 / SiO 2 particles. After applying 5 V the field was removed (OFF) and the color was observed to approach its initial state. The scale bar is 5 mm. Reuse Permissions

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  • Aggregate stability and magnetic characteristics of

    May 20 2017 · Composite Fe m O n –SiO 2 particles have been obtained by precipitation of iron oxide from aqueous solution with the addition of tetraethoxysilane. The shapes and sizes of separate single particles and their aggregates have been determined by scanning electron microscopy. Changes in the stability of the colloidal suspension due to external magnetic field and the addition of NaCl have The composite layers formed by drying a Fe 3 O 4 -SiO 2 -based colloidal solution were studied. The colloidal solution was obtained by the precipitation of Fe 3 O 4 in the presence of highly dispersed silicon dioxide synthesized by the sol-gel method from a tetraethoxysilane alcohol solution. The microstructure and composition of the layers were analyzed using scanning electron microscopy

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  • Magnetochromatic Microspheres Rotating Photonic Crystals

    Fe 3 O 4 SiO 2 core/shell colloids were then prepared through a modified Stöber process. The magnetic colloids and photoinitiator DMPA (5 wt ) were dispersed in PEGDA-700 to form a brown homogeneous solution with a Fe 3 O 4 concentration of 8 mg/mL. In a typical process 1.5 mL of PEGDA precursor solution were mixed with 21 mL of mineral oil Jul 27 2020 · Representative images of the observed structural color response as a function of voltage for each concentration of Fe 2 O 3 / SiO 2 particles. After applying 5 V the field was removed (OFF) and the color was observed to approach its initial state. The scale bar is 5 mm. Reuse Permissions

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  • The Investigation of Superparamagnetic Colloidal Particles

    Colloidal particles based on iron oxides and silica were obtained by sol-gel method. Hysteresis curves at various temperatures were built by MPMS SQUID VSM. Theoretically calculated values of samples remanent magnetization were compared to experimental data. Despite of the average particles size about 10 nm sample has remanent magnetic moment. 2. Experimental details Fine particles of Li0.35 Cd0.3 Fe2.35 O4 /nano SiO2 have been prepared by the sol–gel technique. Analytical grades of Fe(NO3 )3 ·9H2 O LiNO3 ·3H2 O Cd(NO3 )2 ·4H2 O in the required molar ratios as per composition and nano SiO2 in wt were dissolved in ethylene glycol with the addition of water at about 40 C.

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  • Magnetorheology of a magnetic fluid based on Fe3O4

    Clearly the viscosities of MSiNP magnetic fluids are 4.8 times (10 wt ) and 4.2 times (20 wt ) higher than the Fe 3 O 4 magnetic fluid under zero field. The maximum viscosities are 8 times for 10 wt MSiNPs and 25 times for 20 wt MSiNPs compared to the Fe 3 O 4 magnetic fluid. Request PDF Microstructure and magnetic properties of colloidal cobalt nano-clusters The magnetic response of nanometer sized Co nanoparticles

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  • Aggregate stability and magnetic characteristics of

    Composite FemOn–SiO2 particles have been obtained by precipitation of iron oxide from aqueous solution with the addition of tetraethoxysilane. The shapes and sizes of separate single particles and their aggregates have been determined by scanning electron microscopy. Changes in the stability of the colloidal suspension due to external magnetic field and the addition of NaCl have been evaluated. Jan 14 2008 · After the magnetic properties of SiO 2 /Fe 3 O 4 microspheres have been proved we attempted to fabricate a 3D colloidal crystal by self-assembling the magnetic SiO 2 /Fe 3 O 4 microspheres under a magnetic field. The reflection spectrum of the SiO 2 /Fe 3 O 4 magnetic microspheres with a diameter of 700 nm is measured. A 1 kW halogen lamp

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  • Microstructure and magnetic properties of ultrathin FePt

    Dec 21 2018 · To confirm this assumption spectra of FePt-SiO 2 interface region SiO 2 boundary phase and Fe 2 O 3 reference nanoparticles were collected under the same experimental conditions. The FePt-SiO 2 interface spectrum was well fit by the combining the reference spectra of SiO 2 and Fe 2 O 3 using Multiple Linear Least-Square (MLLS) fitting as Figure 1(c) shows the TEM image of the magnetic Fe 3 O 4 NRs SiO 2. Due to the existence of the silica protection layer the iron oxide core successfully maintains the rod structure. The size of the magnetic Fe 3 O 4 NRs SiO 2 is measured to be 349 ± 8 nm in length and 139 ± 4 nm in width. The slight size shrinkage is due to the dehydration

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  • Magnetic properties of FemOn-SiO2 colloidal nanoparticles

    The experimental and theoretical study of FemOn−SiO2 colloidal nanoparticles obtained with various techniques were provided. Aggregation processes for both the techniques were revealed. Nanoparticles have similar average sizes but possess quiet different static magnetic properties including saturation magnetic moment per unit mass and coercive force. A simple sol-gel method was used to prepare magnetic Fe 3 O 4 /SiO 2 /TiO 2 composites with core-shell structure. Fourier transform infrared spectroscopy (FT-IR) X-ray diffraction (XRD) field emission scanning electron microscopy (FE-SEM) and transmission electron microscopy (TEM) have been applied to investigate the structure and morphology of the resultant composites.

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  • Magnetic properties of Fe2O3 nanoparticles embedded in

    Magnetic properties of Fe 2O 3 nanoparticles embedded in hollows of periodic nanoporous silica A. Zeleňáková 1 a J. Kováč 2 and V. Zeleňák3 1Department of Solid State Physics P.J. Šafárik University 04154 Košice Slovakia 2Institute of Experimental Physics Slovak Academy of Sciences 040 01 Košice Slovakia 3Department of Inorganic Chemistry P.J. Šafárik University 04154 Evidence for Fe-Si-O liquid immiscibility at deep Earth pressures Sarah M. Arvesona 1 Jie Deng a Bijaya B. Karkib and Kanani K. M. Lee aDepartment of Geology Geophysics Yale University New Haven CT 06511 and bSchool of Electrical Engineering Computer Science Department of Geology Geophysics Center for Computation and Technology Louisiana State University Baton Rouge LA

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