Volume Fraction Of Nanocrystals Research Articles

Effect of the volume fraction of nanocrystals on the mechanical properties of (Fe0·9Ni0.1)86B14 amorphous/nanocrystalline alloy

The effect of the volume fraction of nanocrystals on the macroscopic mechanical properties and microscopic atomic structure of Fe-based nanocrystalline alloys, as well as the relationship between the two, is an urgent issue to be explored. Seven nanocrystalline alloys with different volume fractions of nanocrystals were formed by annealing treatment of (Fe0·9Ni0.1)86B14 amorphous precursor. Through hardness, flat plate bending, and nanoindentation experiments, it is found that when the volume fraction of nanocrystals reaches the range of 45–55 %, there is an abrupt change in the macroscopic mechanical properties. Specifically, when the volume fraction is less than this range, the properties inherit the amorphous matrix, however, larger than this range, the properties are dominated by precipitated nanocrystalline phases. Meanwhile, based on the molecular dynamics simulation method, seven Fe90Ni10 amorphous nanocrystalline models with different volume fractions of body-centered cubic nanocrystals are established, and the deformation mechanism of models and the evolution of their microstructures during the nanoindentation process are obtained intuitively. Moreover, it is further revealed that the significant changes in the Voronoi polyhedral index, which represents the microscopic atomic structure in this range of nanocrystal volume fractions, are the main reason for the abrupt changes in the mechanical properties at the macroscopic level.

Enhanced Reception and Transmission Performance of Magnetoelectric Antennas With the Optimal Volume Fraction of Nanocrystals

Enhanced Reception and Transmission Performance of Magnetoelectric Antennas With the Optimal Volume Fraction of Nanocrystals

The effect of the volume fraction of nanocrystals on the brittleness of Fe-based amorphous/nanocrystalline alloys simulated by molecular dynamics

The effect of the volume fraction of body-centered cubic (BCC) crystal in Fe-based amorphous nanocrystalline alloys on room temperature brittleness was investigated via molecular dynamics simulations. Seven model samples with embedded BCC nanocrystal contents ranging from 0 to 33.4 vol.% were obtained. The indentation tests were carried out by spherical rigid indenter to investigate the microstructural evolution and the mechanical properties of those Fe-based amorphous/nanocrystalline alloys in terms of the indentation force, hardness, von Mises shear strain, atomic displacement vector as well as surface morphology. It is found virtually that the plasticity shows a gradient decrease tendency for the three types of samples with 0, less than 16, and more than 20 vol.% nanocrystal, respectively, which is caused by the free volume decreases via monitoring the Voronoi polyhedra.

Influence of amorphous phase on coercivity in SmCo5-Cu nanocomposites

Severe plastic deformation of powder blends consisting of SmCo5-Cu results in magnetically hardened nanocomposite bulk materials. Previously it was reported that the microstructure is continuously refined with increasing deformation, yet, coercivity saturates at a certain level of strain and partial amorphization of the SmCo5 phase is observed. In this work larger strains, over the range of the previous work are applied showing further structural refinement but a strong decrease in coercivity. Micromagnetic simulations based on the experimentally observed microstructure serve to clarify the effect of amorphization in the SmCo5 phase and disclose the detrimental character of the amorphous phase. For a fixed volume fraction of nanocrystals the simulations reveal an increasing coercivity with decreasing the size of them due to increasing number of interfaces acting as pinning sites. Furthermore, our micromagnetic simulations disclose the mechanisms of saturation and decline of magnetic hardening due to the strain induced by high-pressure torsion.

Investigation of LSPR Coupling Effects toward the Rational Design of CsxWO3–δ Based Solar NIR Filtering Coatings

AbstractThe optical range of localized surface plasmon resonance (LSPR) is extended into the infrared region, thanks to the development of highly doped semiconductor nanocrystals. Particularly, the near‐infrared (NIR) range holds a significant interest in managing solar radiation. However, practical applications necessitate the arrangement of particles, which is known to possibly impact their optical properties through LSPR coupling effects. How such coupling modifies the LSPR response in semiconductor hosts remains largely unexplored. In this study, a protocol for producing composite coatings composed of cesium‐doped tungsten bronze nanocrystals embedded in a silica matrix is presented. Achieving individual dispersion of nanocrystals is made possible through careful selection of a surface polyglycerol ligand exchange. This allows to tune the interparticle distance by adjusting the nanocrystal volume fraction in the composite. The findings demonstrate that LSPR coupling effects significantly influence the LSPR intensity of nanocrystals in the composite when the nanocrystal‐to‐nanocrystal distance matches their size. Beyond elucidating the LSPR coupling effect, this study provides insights into the potential use of Cs‐HTB nanocrystals for solar control applications. Through the optimization of morphology and film structure, remarkable selectivity is obtained in terms of maintaining good transparency in the visible range while achieving high absorption in the NIR.

Effect of Isothermal Treatment on Microstructure and Performance of Micro/Nanostructure 2205 Duplex Stainless Steel Prepared by Aluminothermic Reaction

Using an appropriate heat treatment process to control the precipitation of the σ phase, while regulating the alloy structure and grain size, is one of the effective ways to obtain good comprehensive properties of duplex stainless steel (DSS). Herein, the feasibility and preparation parameters of micro/nanostructure 2205 DSS prepared by the aluminothermic reaction are explored. The microstructure and properties are further controlled by isothermal treatment at 1000 °C for a different time. The results show that the volume percentages of α and γ phases in the 1.0 h isothermal treated steel obtain a maximum value and a minimum value, corresponding to 60% and 36%, respectively. The evolution of microstructure with isothermal treatment also affects the content and morphology of the precipitated σ phase, which changes from continuous precipitation to granular precipitation at the α/γ phase boundaries, and its volume percentage obtains a minimum value when the isothermal treatment is performed for 1.0 h. With the increase of heat treatment time, the average grain size and volume fraction of nanocrystals increase gradually. Corresponding to the changes in microstructure and grain size, the maximum values of Vickers hardness and tensile properties of the alloy are obtained after 1.0 h isothermal treatment.

Liquid-Phase Synthesis, Sintering, and Transport Properties of Nanoparticle-Based Boron-Rich Composites

Nanostructuring boron-rich materials should significantly impact their thermal and electrical transport properties. Nonetheless, nanostructured monoliths of such materials could not be achieved in the 10 nm range so far, because of the large temperatures required to synthesize and produce boron-rich compounds. Such a nanostructuration may have important consequences for achieving a trade-off between enhanced electrical and low thermal conductivity in boron-rich materials, which are among the few materials enabling thermoelectric power generation above 1000 K thanks to their thermal stability, high positive Seebeck coefficients, and low thermal conductivity. In this study, we use a one-pot synthesis in inorganic molten salts to yield a nanocomposite consisting of metallic HfB2 nanocrystals dispersed in an insulating amorphous boron-rich matrix with a controlled volume fraction of nanocrystals from 16 to 56 vol %. We show that this controlled liquid-phase synthesis can be coupled to spark plasma sintering for densification preserving the nanostructure. The relationships between the reagent ratio in the liquid-phase synthesis, sintering conditions, and transport properties of the densified nanocomposites are then highlighted. We then design materials exhibiting metallic electrical conductivity related to the HfB2 nanocrystals, together with enhanced thermal dissipation attributed to the nanostructured amorphous boron matrix. Combined with the versatility offered by in-solution routes toward boride-based nanocomposites, this work opens a new avenue for tuning transport properties in boron-rich nanomaterials.

Modeling atomic layer deposition process parameters to achieve dense nanocrystal-based nanocomposites

Atomic layer deposition (ALD) is a technique capable of depositing conformal coatings in highly tortuous 3D nanostructures. One configuration that has attracted attention is nanocrystal (NC) based nanocomposite films, whereby a 3D network of randomly packed nanocrystals is infilled via ALD to yield a dense nanocomposite. In this work, we demonstrate criteria for predicting three important thermal ALD process parameters necessary to completely infill 3D NC networks: cycle number, precursor pulse time, and purge time. A description of representative pore geometry is developed using parameters of the film comprised of nanocrystals before infill, specifically NC diameter, NC volume fraction, and film thickness. This geometric description allowed for prediction of required precursor pulse times to saturate the NC film surface. A finite-difference model of water vapor transport during purging revealed that desorption kinetics can be used to predict purge times required to achieve complete infill. The model predictions show good agreement with experiments carried out by infilling films comprised of GaN NCs with ZnO by the diethylzinc/water process and films comprised of Al2O3 NCs with Al2O3 by the trimethylaluminum/water process.

Anomalously low Rayleigh scattering by CdS/CdSe doped glasses

Light scattering (Raman, Rayleigh and Mandelshtam-Brillouin) and absorption of commercial color glasses (cut-off optical filters containing nanocrystals of ternary compounds CdSxSe1–x) were studied. It was found for the first time that the contribution of nanocrystals to the Rayleigh scattering is unprecedentedly low for some of these glasses. This conclusion is confirmed by estimation of nanocrystal size and volume fraction from low-frequency Raman scattering and absorbance spectroscopy for a chosen set of samples. Anomalously low Rayleigh scattering of nanocrystals is explained in terms of interference of light scattered by different nanocrystals (interparticle interference). The possibility of interparticle interference effects in the case of small volume fraction of nanocrystals is illustrated by computer simulation using the model of diffusion-limited phase transformation proposed earlier.

Influence of Ni substitution for B on crystallization behavior, microstructure and magnetic properties of FeBCu alloys

Abstract The crystallization, microstructure and magnetic properties of Fe83NixB16−xCu1 (x = 0, 1, 2, 4) alloys are investigated by Mossbauer spectroscopy, X-ray diffractometry and magnetometry. The substitution of Ni for B in the Fe83B16Cu1 alloy enriches Fe clusters in melt-spun ribbons and promotes the nucleation of α-Fe(Ni), which is beneficial to the formation of high volume fraction of nanocrystals after crystallization. Furthermore, the addition of 1–2 at.% Ni widens the annealing temperature range for the alloys with low HC. Excellent magnetic properties with high saturation magnetic flux density (BS) of 1.83 T and low coercivity (HC) of 9.2 A/m are obtained by annealing the Fe83Ni2B14Cu1 melt-spun ribbons. In addition, the nanocrystalline alloy with x = 2 possesses a lower saturation magnetostriction (19 ppm) than that of the Ni-free alloy (25 ppm).

Crystallization of Nanocrystals in Spherical Confinement Probed by in Situ X-ray Scattering.

We studied the formation of supraparticles from nanocrystals confined in slowly evaporating oil droplets in an oil-in-water emulsion. The nanocrystals consist of an FeO core, a CoFe2O4 shell, and oleate capping ligands, with an overall diameter of 12.5 nm. We performed in situ small- and wide-angle X-ray scattering experiments during the entire period of solvent evaporation and colloidal crystallization. We observed a slow increase in the volume fraction of nanocrystals inside the oil droplets up to 20%, at which a sudden crystallization occurs. Our computer simulations show that crystallization at such a low volume fraction is only possible if attractive interactions between colloidal nanocrystals are taken into account in the model as well. The spherical supraparticles have a diameter of about 700 nm and consist of a few crystalline face-centered cubic domains. Nanocrystal supraparticles bear importance for magnetic and optoelectronic applications, such as color tunable biolabels, color tunable phosphors in LEDs, and miniaturized lasers.

Evolution of Microstructure and Incorporation of Excess Hydrogen During the Growth of Hydrogenated Polymorphous Silicon at High Rate

Hydrogenated polymorphous silicon (pm-Si:H) is a material consisting of a small volume fraction of nanocrystals embedded in an amorphous matrix, and which can be grown at high deposition rates by increasing the radio-frequency power. When grown at high deposition rates, pm-Si:H films show a shift of their infrared (IR) absorption stretching band peak to higher wavenumbers and a sudden increase in their optical bandgap. The IR absorption spectrum was analyzed by deconvolution into three bands, including a medium stretching mode positioned at 2030 cm−1, which has been attributed to Si–H bonds at silicon nanocrystal surfaces. Secondary ion mass spectrometry measurements confirmed that an excess of hydrogen is incorporated in pm-Si:H grown at high deposition rate, leading to a sharp increase in the optical bandgap. We suggest that this sharp increase can be used as a simple tool to detect the deterioration of material quality when using high deposition rate processes.

Low Temperature Fluorinated Silicon FILMS Synthesis

Second-harmonic generation (SHG), photoluminescence (PL) and Fourier-transformed infrared (FT IR) spectra from silicon films with different average size of nanocrystals were analized to develop new possible material for active channel in nonlinear optical devices. Silicon films were prepared with dominant concentrations of silicon bonding with oxygen or fluorine atoms. Also, the volume fraction of nanocrystals was varied from 30% to 70%. It is seen the spectral peak with energy 3.26 eV is related to defects appeared in interface area silicon-silicon dioxide. For films with small silicon crystals (less than 20 nm) the nonlinear optical response contains two spectral peaks. The second peak is caused by optical response from nanocrystal grain boundary that contains oxygen or fluorine atoms incorporated in silicon as dipoles inside film. The optical nonlinear switch device based on the nonlinear optical response of SiOxmedia inside film was proposed. Also, the silicon film with quartz micro-clusters was investigated as material for making the nonlinear optical transmitter device. The structural properties of silicon films can be easily illustrated by using the films morphology which was determined by using atomic-force microscopy. Figure 1 shows the atomic-force microscopic photos for Sample 1, Sample 2 and Sample3, respectively. It is seen, that the nanocrystal grains are in all types of investigated silicon films. The lateral distribution of nanocrystals with dominant orientation (111) are homogeneous for Sample 1 (see Fig. 1 a)), but for the Sample 2 is unhomogeneous due to appeared conglomerates which are created from the amorphous phase separately (see Fig. 1 b)). The Sample 3 has the triangular shape of nanocrystals (111) which are distributed in submicron crystalline (111) domens. It is clear, that there is great difference in morphological properties of three types of films. The HF etching the silicon surface is efficient because at Td=100oC the surface diffusion and desorption from the surface are low. By adding the SiF4 we change the H2 :SiF4 ratio and some amount of fluorine atoms are included into H2SiF6 assembly creation. Because, the etching process is low at [SiF4] =0.25 sccm and [SiF4] =0.375 sccm. After this values of silicon tetra-fluoride flow rate the H2:SiF4 ratio is changed to destruct intensive creation of molecular assemblies. This stage at [SiF4] =0.5 sccm the HF significant etches the silicon and causes the decreasing the grain sizes. It is assumed that there are two possibilities of fluorine removing: the first is hydrogen incorporation with fluorine, and, the second, the H2SiF6 assemble is creation by 300oC. The SHG is forbidden for centrosymmetric crystal such as bulk silicon because the sum dipole moment is zero, but it is possible due to the surface breaking symmetry and quadruple terms contributions. The opposite situation is for nanostructured oxidized (or fluorinated) silicon films for which the surface area of great quantity of nanocrystals is significant, and the breaking of symmetry is permanent and lateral isotropic. The spectral characteristic of optical nonlinear response from the thin silicon film strictly depends on the spectral properties of polarization and susceptibility tensors χ(2) distortion and χ(2) Si-O.F are the nonlinear susceptibilities produced by nonzero dipole moment caused by shape distortion from the spherical shape of nanocrystals and due to the existing of dangling bonds caused by fluorine or oxygen incorporation in grain boundary region, respectively. By these values of densities the dipole moments of such nanoscaled ellipsoidal dipoles covered by surface charges can be estimated as PSiO =0.04 Debye and PSiH =0.015 Debye. Therefore, the concentration of nanocrystals mainly plays a great role in PL and SHG signal intensity of radiation due to their great surface area covered by silicon bonds with contaminants (atoms of O, H, F) in grain boundary but not as a separate nanoscaled dipoles. By increasing the nanocrystal quantity inside the silicon film the ratio S/V grows significant. The size effect in PL from nanocrystalline silicon film can be explained by means of statistical method. We suggested that the ƒ(x) is distribution function of crystallites in their sizes, θ(x) is a quantum efficiency of nanocrystalls. It is supposed, that the large quantity of nanocrystals is Gauss distributed in their sizes. The Nnc-Si value is proportional to the square under the both functions ƒ(x) and θ(x) near the zero values. Accordingly, the quantity of emitted hydrogenized nanocrystals by band-to-band radiative transitions is important to esimate the PL linear optical response. For nanocrystalline silicon films for Pin àSout optical scheme χ(2) xxx component of susceptibility tensor is detected. By using optical scheme Pin àPout SHG spectra contains isotropic and anisotropic component of susceptibility tensor χ(2) zzz, χ(2) zxx,χ(2) xxz , and χ(2) xxx. Figure 1

Light-induced changes in silicon nanocrystal based solar cells: Modification of silicon–hydrogen bonding on silicon nanocrystal surface under illumination

Hydrogenated polymorphous silicon (pm-Si:H) is a material consisting of a small volume fraction of nanocrystals embedded in an amorphous matrix. pm-Si:H solar cells demonstrate interesting initial degradation behaviors such as rapid initial change in photovoltaic parameters and self-healing after degradation during light-soaking. The precise dynamics of the light-induced degradation was studied in a series of light-soaking experiments under various illumination conditions such as AM1.5G and filtered 570 nm yellow light. Hydrogen effusion experiment before and after light-soaking further revealed that the initial degradation of pm-Si:H solar cells originate from the modification of silicon–hydrogen bonding on the surface of silicon nanocrystals in pm-Si:H.

(Invited) Colloidal Nanocrystal Composites with High and Low Thermal Conductivity

We present our work on thermal transport in colloidal nanocrystal composites within the context of thermoelectrics and thermal energy management. Colloidal nanocrystals consist of an inorganic crystalline core with short ligand molecules bound to the surface. These nanocrystals can be made with excellent control over size, shape, and composition, thereby enabling microstructural control over thermal energy transport. Our first two topics focus on low thermal conductivity materials for thermoelectricity: semiconductor nanocrystal thin films and semiconductor matrix – semiconductor nanoparticle composites. Our last topic focuses on metal matrix – metal nanoparticle composites with high thermal conductivity, which can be used to thermally manage transient power spikes in high power electronics. For the first topic, we systematically study the effect of nanocrystal diameter and surface chemistry on thermal transport in lead chalcogenide nanocrystal thin films. These samples exhibit very low thermal conductivities ranging from 0.1 to 0.5 W/m-K and we find that larger nanocrystals and shorter ligands generally lead to higher thermal conductivities. Our measurements also show that the effect of surface chemistry on thermal transport becomes more pronounced as nanocrystal diameter decreases. For the second topic, we focus on polycrystalline In2Se3 matrices with embedded CdSe nanocrystals ranging from 0 to ~100 vol%. We find that the thermal conductivities of these composites are very low over the entire nanocrystal volume fraction range and vary from 0.3 to 0.5 W/m-K. We also find that the presence of CdSe nanocrystals strongly effects the formation of the In2Se3 matrix (i.e. grain orientation and size as well as ternary phase formation). Lastly, we present our work on phase change Bi nanocrystals embedded in a solid Ag-matrix. The latent heat of the phase change Bi nanocrystals can absorb large quantities of transient heat generated during power spikes in power electronics operation. In addition, fast thermal energy transport is facilitated by the Ag-matrix, which leads to high composite thermal conductivities ranging from 101 to 102 W/m-K. We also use size-dependent melting of the phase change nanocrystals as a design variable for the thermal energy absorption temperature.

Effects of nanocrystals on evolution behavior of shear transformation zones in Zr85Cu15 metallic glasses

Structural evolution sites induced by shear stress and annealing were investigated via molecular dynamic simulations using a Zr85Cu15 metallic glass (MG) system. The crystalline phase induced by annealing occupies the preferred sites of shear transformation zones (STZs), forcing STZ formation in other parts of the amorphous matrix through deformation. This process fundamentally alters the path of shear bands in nanocrystal MGs. Meanwhile, more STZs are activated in the rest of the parts of the amorphous matrix when the volume fraction of nanocrystals is 13.5%, significantly enhancing the plasticity of nanocrystal-MGs. Our study may provide novel insights regarding the plastic deformation mechanism of nanocrystal MGs at the atomic scale.

Far-infrared spectroscopic study of CeO2 nanocrystals

We present the far-infrared reflectivity spectra of 5 nm-sized pure and copper-doped Ce1−xCuxO2−y (x = 0; 0.01 and 0.10) nanocrystals measured at room temperature in the 50–650 cm−1 spectral range. Reflectivity spectra were analyzed using the factorized form of the dielectric function, which includes the phonon and the free carriers contribution. Four oscillators with TO energies of approximately 135, 280, 370, and 490 cm−1 were included in the fitting procedure. These oscillators represent local maxima of the CeO2 phonon density of states, which is also calculated using the density functional theory. The lowest energy oscillator represents TA(L)/TA(X) phonon states, which become infrared-active Eu modes at the L and X points of the Brillouin zone (BZ). The second oscillator originates from TO(Γ) phonon states. The oscillator at ~400 cm−1 originates from Raman mode phonon states, which at the L point of BZ also becomes infrared-active Eu mode. The last oscillator describes phonons with dominantly LO(Γ) infrared mode character. The appearance of phonon density of states related oscillators, instead of single F2uinfrared-active mode in the far-infrared reflectivity spectra, is a consequence of the nanosized dimension of the CeO2 particles. The best fit spectra are obtained using the generalized Bruggeman model for inhomogeneous media, which takes into account the nanocrystal volume fraction and the pore shape.

Processing and Characterization of Amorphous/Nanocrystalline Al87.5Ni4Sm8.5 Particles Reinforced Crystalline Al Matrix Composites

Metal matrix composites, in which crystalline Al was reinforced by particulates of the Al87.5Ni4Sm8.5 amorphous alloy, were produced using cold pressing and hot extrusion processing. Controlled nanoprecipitation was used to improve the mechanical properties of the amorphous alloy. Amorphous melt-spun ribbons were produced by melt-spinning technique and then fragmented in fine powder by high-energy ball milling. Amorphous and pure aluminum powders were mixed in two different proportions: 85:15 and 70:30 (wt%) and homogenized by ball milling. Bulk samples were produced via cold pressing and hot extrusion. Controlled nanoprecipitation within the amorphous alloy was obtained by the correct choice of processing temperature. The composites were analyzed for reinforcement distribution, porosity content, microhardness and compression tests. The results showed that it was possible to control the precipitation by producing almost the same volume fraction of nanocrystals in each condition. Compression tests showed an improvement on the mechanical properties, which were correlated with the presence of the amorphous/nanocrystals reinforcement in the Al-matrix. The compression yield-strengths of the as-extruded composites were 192 and 310 MPa for 15% and 30% in volume of Al87.5Ni4Sm8.5, respectively. These values are significantly higher than the typically found for the AA1100 wrought pure aluminum (180 MPa).

Homogeneous viscous flow behavior of a Cu–Zr based bulk metallic glass composites

Abstract In this paper, Cu40Zr44Ag8Al8 bulk metallic glass composites (BMGCs) consisting of various volume fraction of nanocrystals embedded in the amorphous matrix was synthesized by controlled annealing treatment of an as-cast BMGCs. The high temperature compression behaviors of the BMGCs were characterized in the supercooled liquid region. Results show that the flow stresses keep increasing after an initial decrease with extension of the annealing time. With annealing the values of activation volume Vact is determined to be increasing from 283.6216 Ǻ3 to 305.553 Ǻ3, suggesting that the jump of atoms is a cooperative process during the high-temperature deformation. Flow behavior of the BMGCs annealed for less than 8 min transform from Newtonian to non-Newtonian dependant on the stain rate and can be successively fitted by the visco-plasticity model. Fitting results indicate that deformation behaviors of these samples are governed by homogeneous flow of the amorphous matrix and indeed determined by the viscosities in the Newtonian flow stage. However, the BMGCs annealed for 8 min exhibit a non-Newtonian flow over the entire compression process and fail to be fitted by the visco-plasticity model. Micrographs of the sample reflect an impinged structure, indicating that high temperature deformation behavior of the BMGCs with high volume fractions of particles is indeed controlled by that of a backbone of particles.

Measurement of Thermal Conductivity of PbTe Nanocrystal Coated Glass Fibers by the 3ω Method

Fiber-based thermoelectric materials can conform to curved surfaces to form energy harvesting devices for waste heat recovery. Here we investigate the thermal conductivity in the axial direction of glass fibers coated with lead telluride (PbTe) nanocrystals using the self-heated 3ω method particularly at low frequency. While prior 3ω measurements on wire-like structures have only been demonstrated for high thermal conductivity materials, the present work demonstrates the suitability of the 3ω method for PbTe nanocrystal coated glass fibers where the low thermal conductivity and high aspect ratio result in a significant thermal radiation effect. We simulate the experiment using a finite-difference method that corrects the thermal radiation effect and extract the thermal conductivity of glass fibers coated by PbTe nanocrystals. The simulation method for radiation correction is shown to be generally much more accurate than analytical methods. We explore the effect of nanocrystal volume fraction on thermal conductivity and obtain results in the range of 0.50-0.93 W/mK near room temperature.