“…[48] In this case, H c increases with crystal size. [3,5] EM properties EM parameters and their matching were studied to reveal the microwavea bsorbing mechanism of Cu x Fe 3Àx O 4 @Cu composites. As shown in Figure 7, the EM parameters are affected by the composition of all Cu x Fe 3Àx O 4 @Cu composites within 2-18 GHz.…”
“…However, the high density and low permittivity of spinelf errites limit their application as light and thin absorption materials. Light absorption materials can be prepared by using two approaches:i )decreasing the absorber density by selecting hollow or porous structures [3,4] or decreasing the particle size to nanoscale [5] and ii)improving EM parameters to reduce the filling mass or volume fraction of the absorbers in the matrix. [6] Permittivity can be enhanced with the followings trategies:i )enhancement of space charge, ori-entation, or interface polarizationsb ym odulating the dimension, morphology, composition, and structure of absorbents; [7,8] using nanomaterials with low percolation threshold to form microcurrents through an electrical percolation network; [9,10] ii) selection of plasmonic structures( i.e.,r ings) as absorbers to generate plasmonic resonance-enhanced permittivity; [11,12] and iii)surface modification of the particles using other materials with high permittivity.…”
“…[48] In this case, H c increases with crystal size. [3,5] EM properties EM parameters and their matching were studied to reveal the microwavea bsorbing mechanism of Cu x Fe 3Àx O 4 @Cu composites. As shown in Figure 7, the EM parameters are affected by the composition of all Cu x Fe 3Àx O 4 @Cu composites within 2-18 GHz.…”
“…However, the high density and low permittivity of spinelf errites limit their application as light and thin absorption materials. Light absorption materials can be prepared by using two approaches:i )decreasing the absorber density by selecting hollow or porous structures [3,4] or decreasing the particle size to nanoscale [5] and ii)improving EM parameters to reduce the filling mass or volume fraction of the absorbers in the matrix. [6] Permittivity can be enhanced with the followings trategies:i )enhancement of space charge, ori-entation, or interface polarizationsb ym odulating the dimension, morphology, composition, and structure of absorbents; [7,8] using nanomaterials with low percolation threshold to form microcurrents through an electrical percolation network; [9,10] ii) selection of plasmonic structures( i.e.,r ings) as absorbers to generate plasmonic resonance-enhanced permittivity; [11,12] and iii)surface modification of the particles using other materials with high permittivity.…”
“…Previous studies have shown that the high crystallite size in nanocubes leads to high saturation magnetization because of reduced surface spin disorder. 13 , 31 , 50 Liu et al varied the crystal size and showed that for polycrystalline nanospheres less than 250 nm in size, the saturation magnetization depends on both the diameter and its crystal size (and hence crystallinity). 50 As expected, 50 , 51 owing to the higher crystal size in the multidomain MNPs, the saturation magnetization of Fe 3 O 4 nanocubes is higher than that of nanospheres ( Tables 1 – 3 ).…”
This paper highlights the relation
between the shape of iron oxide
(Fe3O4) particles and their magnetic sensing
ability. We synthesized Fe3O4 nanocubes and
nanospheres having tunable sizes via solvothermal and thermal decomposition
synthesis reactions, respectively, to obtain samples in which the
volumes and body diagonals/diameters were equivalent. Vibrating sample
magnetometry (VSM) data showed that the saturation magnetization (Ms) and coercivity of 100–225 nm cubic
magnetic nanoparticles (MNPs) were, respectively, 1.4–3.0 and
1.1–8.4 times those of spherical MNPs on a same-volume and
same-body diagonal/diameter basis. The Curie temperature for the cubic
Fe3O4 MNPs for each size was also higher than
that of the corresponding spherical MNPs; furthermore, the cubic Fe3O4 MNPs were more crystalline than the corresponding
spherical MNPs. For applications relying on both higher contact area
and enhanced magnetic properties, higher-Ms Fe3O4 nanocubes offer distinct advantages
over Fe3O4 nanospheres of the same-volume or
same-body diagonal/diameter. We evaluated the sensing potential of
our synthesized MNPs using giant magnetoresistive (GMR) sensing and force-induced remnant magnetization
spectroscopy (FIRMS). Preliminary data obtained by GMR sensing confirmed
that the nanocubes exhibited a distinct sensitivity advantage over
the nanospheres. Similarly, FIRMS data showed that when subjected
to the same force at the same initial concentration, a greater number
of nanocubes remained bound to the sensor surface because of higher
surface contact area. Because greater binding and higher Ms translate to stronger signal and better analytical sensitivity,
nanocubes are an attractive alternative to nanospheres in sensing
applications.
“…Generally, since the approach of wet chemistry methods is aggregation of atoms produced in solution into nanoparticles, good control of the reaction, of the size of the particles, and the size distribution may be achieved. The most widely used methods of iron oxide nanostructuring are thermal decomposition [9,10], sometimes combined with the polyol process [11,12], and solvothermal method [13,14,15,16], where polyols may also be used as well. Some of the most common precursors that have been used in iron oxide nanostructuring are iron (II) acetylacetonate [17], iron oleate [18], iron (II) acetate [19], iron nitrate nonahydrate [20], and iron pentacarbonyl [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…Generally, this method offers a wide range of reaction temperature values, considering that any long-chain polyol has a different boiling point, which depends on the relative molecular mass, leading to the control of the physicochemical characteristics of the nanoparticles such as crystal phase and size. Magnetite particles in a size range between 82 and 1116 nm have been prepared by Liu et al [14] by using ethylene glycol (EG). Longer-chain polyols such as triethylene glycol (TrEG) have been used in magnetite nanostructuring [14,15] as well, while even longer polyethylene glycols (PEGs) resulted to same phase nanoproducts [15,16].…”
A study of the influence of polyols, with or without an additional reducing agent, on crystallites’ size and magnetic features in Fe3O4 nanoparticles and on their performance in magnetic particle hyperthermia is presented. Three different samples were synthesized by thermal decomposition of an iron precursor in the presence of NaBH4 in a polyol. So far, triethylene glycol (TrEG) and polyethylene glycol (PEG 1000 and PEG 8000) that exhibit different physical and chemical properties have been used in order to investigate the influence of the polyols on the composition and the size of the NPs. Additionally, the presence of a different reducing agent such as hydrazine, has been tested for comparison reasons in case of TrEG. Three more samples were prepared solvothermally by using the same polyols, which led to different crystallite sizes. The magnetic core of the nanoparticles was characterized, while the presence of the surfactant was studied qualitatively and quantitatively. Concerning the magnetic features, all samples present magnetic hysteresis including remanence and coercivity revealing that they are thermally blocked at room temperature. Finally, a study on the influence of the MNPs heating efficiency from their size and the field amplitude was accomplished. In our polyol process the main idea was to control the specific loss power (SLP) values by the nanoparticles’ size and consequently by the polyol itself.
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