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At least 325 records · Page 18

Multi-scale time-resolved electron diffraction: A case study in moiré materials

Ultrafast-optical-pump — structural-probe measurements, including ultrafast electron and x-ray scattering, provide direct experimental access to the fundamental timescales of atomic motion, and are thus foundational techniques for studying matter out of equilibrium. High-performance detectors are needed in scattering experiments to obtain maximum scientific value from every probe particle. Here we deploy a hybrid pixel array direct electron detector to perform ultrafast electron diffraction experiments on a WSe 2 /MoSe 2 2D heterobilayer, resolving the weak features of diffuse scattering and moiré superlattice structure without saturating the zero order peak. Enabled by the detector’s high frame rate, we show that a chopping technique provides diffraction difference images with signal-to-noise at the shot noise limit. Finally, we demonstrate that a fast detector frame rate coupled with a high repetition rate probe can provide continuous time resolution from femtoseconds to seconds, enabling us to perform a scanning ultrafast electron diffraction experiment that maps thermal transport in WSe 2 /MoSe 2 and resolves distinct diffusion mechanisms in space and time.

36 MATERIALS SCIENCE↗

Magnetic Properties of Co-doped Bismuth Oxide (δ-Bi{sub 2}O{sub 3}) at Low Temperature

The (Bi{sub 2}O{sub 3}){sub 1−x−y}(Gd{sub 2}O{sub 3}){sub x}(Lu{sub 2}O{sub 3}){sub y} material compounds were prepared by using the solid-state reaction technique under normal air conditions. The heat treatments of the ternary samples were performed firstly at 800 °C for 48 h and then at 750 °C for 100 h. The structural, morphological, and magnetic properties of the materials were characterized by X-ray powder diffraction (XRD), scanning electron microscope, and a Quantum Design PPMS-9T system, respectively. From the XRD results, it was found that the phases of all of the samples consisted of the fluorite-type face-centered cubic δ-Bi{sub 2}O{sub 3} phase. It was observed that the microstructure of the samples is uniformly distributed on the samples’ surface. The temperature dependence of magnetization (M–T) measurements showed that the magnetization rose sharply at the critical temperature. The calculated critical temperature values vary from 22.19 to 56.61 K for the samples. All of the samples displayed the paramagnetic behavior. The paramagnetic behavior started from 300 K to very low temperature which varied from 22.19 to 56.61 K. The coercive rise on the magnetization below 22.19 K or 56.61 K with decreasing temperature causes a phase transformation in the δ-Bi{sub 2}O{sub 3} system. This sudden increment was considered as a ferromagnetic or ferrimagnetic phase transition.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Effect of Cr{sup 3+} Ions Substitution on Structural and Magnetic Properties of Co Ferrite Nanoparticles

A series of polycrystalline nanoferrite having the chemical formula CoCr{sub x}Fe{sub 2−x}O{sub 4} (x = 0.0, 0.2, 0.4, 0.6, 0.8, and 1.0) were synthesized by sol-gel autocombustion method. X-ray diffraction (XRD) analysis was used to investigate the structural parameters and also to check the phase purity of all prepared samples. The analysis of XRD patterns revealed the formation of single-phase cubic spinel structure for all samples. The average particle size of the synthesized ferrites was identified by X-ray diffraction and scanning electron microscopy technique. The magnetic properties of Co-Cr nanoferrites were measured using a hysteresis loop tracer at room temperature and magnetic field of 5 KOe. Saturation magnetization (M{sub s}) and coercivity (H{sub c}) decrease with the increasing Cr{sup 3+} ions concentration in the Co-Cr ferrite, indicating that lesser magnetic Cr{sup 3+} ions substitute Fe{sup 3+} ions in the octahedral sublattice of the ferrite. Such materials are useful to reduce the energy loss in AC electrical appliances.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Magnetic Behavior of Iron-Rich Permalloy Nanoparticles

Iron-rich permalloy Fe{sub x}Ni{sub 1−x} nanoparticles (NPs) were fabricated using a low-temperature wet chemistry method involving the hydrothermal growth of the NPs. Three Fe–Ni NPs (Fe{sub 0.5}Ni{sub 0.5}, Fe{sub 0.625}Ni{sub 0.375}, and Fe{sub 0.83}Ni{sub 0.17}) were fabricated and studied by X-ray diffraction (XRD), scanning electron microscopy (SEM), and vibrating sample magnetometer (VSM). After the initial formations, the three Fe–Ni NPs were annealed at 200, 400, and 600 °C; the XRD showed that all three FeNi NPs had a bcc structure (not the fcc structure of the standard Fe{sub 20}Ni{sub 80} permalloy). The SEM images showed that the NPs had spherical shapes. The VSM measurements showed that none of the Fe–Ni nanoparticles were superparamagnets but were ferromagnets. The heat treatments cause the work needed to the flip the spin (coercivity (H{sub c})) to increase and the values of the saturation magnetizations to fluctuate.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Excess Conductivity Investigation of Y{sub 3}Ba{sub 5}Cu{sub 8}O{sub 18±δ} Superconductors Prepared by Various Parameters of Planetary Ball Milling Technique

Superconducting samples of type Y{sub 3}Ba{sub 5}Cu{sub 8}O{sub 18±δ} were elaborated by using a planetary high-energy ball milling (HEBM) technique with various parameters. Phases, microstructure, and superconductivity have been examined using X-ray powder diffraction (XRD), scanning electron microscopy (SEM), and electrical resistivity measurements. SEM investigation shows the occurrence of nanoentities embedded into the superconducting matrix for samples prepared by a ball milling technique. The main objective of this study is to investigate the influence of ball milling parameters on the fluctuation-induced conductivity (FIC). The electrical resistivity versus temperature, ρ(T), above T{sub c} was analyzed using Lawrence–Doniach (LD) and Aslamazov–Larkin (AL) models. Different fluctuation regimes indicated by short-wave fluctuation (SWF) and three-dimensional (3D), two-dimensional (2D), one-dimensional (1D), and critical region (CR) fluctuations were identified. The coherence length at zero temperature, the effective layer thickness, the critical magnetic fields, and the critical current densities are determined. The superconducting parameters strongly depend on the planetary ball milling technique, and the results are explained in relevancy to the microstructure. It was found that the achievement of a microstructure with well-dispersed nanoentities is an effective way for introducing pinning centers for enhancing critical current density and flux pinning capability of bulk Y-358.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Influence of bath temperatures on physical and electrical properties of potentiostatically deposited Cu{sub 2}O thin films for heterojunction solar cell applications

In the present work, the influence of bath temperatures on structural, morphological, vibrational, optical, electrical and photo response properties of the electrochemically deposited cuprous oxide (Cu{sub 2}O) thin films on fluorine doped tin oxide substrate is extensively investigated with the help of X-ray diffraction (XRD), scanning electron microscopy (SEM), Micro Raman spectroscopy, photo luminescence (PL) spectroscopy, UV–visible spectroscopy, LCR measurement, Keithley 4200 semiconductor characterization system respectively. XRD patterns reveal that the deposited Cu{sub 2}O films have cubic structure grown along the preferential (111) orientation and the film deposited at 40 °C shows better crystalline nature when compared at 55 and 70 °C. The micro structural properties of films such as crystallite size (D), dislocation density (δ), micro strain (ε) and stacking fault probability (α) were calculated and discussed in detail. SEM displays a well-defined three side pyramid shaped morphology for the film deposited at 40 °C. Micro Raman and PL spectra reveal the film deposited at 40 °C by being better crystalline at a higher acceptor concentration. UV–Visible study shows that the optical energy band gap increases from 2.05 to 2.17 eV with an increase in bath temperature from 40 to 70 °C. The frequency-temperature dependence of impedance analysis shows a higher electrical conductivity for a film deposited at 40 °C compared to other bath temperatures. I-V measurement illustrates a good photoconductivity response for Cu{sub 2}O thin film deposited at 40 °C compared to films deposited at 55 and 70 °C.

36 MATERIALS SCIENCE↗

Ultrasound-assisted facile synthesis of a new tantalum(V) metal-organic framework nanostructure: Design, characterization, systematic study, and CO{sub 2} adsorption performance

This work presents a fast route for the preparation of a new Ta(V) metal-organic framework nanostructure with high surface area, significant porosity, and small size distribution. X-ray diffraction (XRD), scanning electron microscopy (SEM), Transition electron microscopy (TEM), energy dispersive spectrometer (EDS), thermo-gravimetric analysis (TGA), differential scanning calorimetry (DSC), fourier transform infrared spectroscopy (FTIR), CHNS/O elemental analyser, and Brunauer-Emmett-Teller (BET) surface area analysis were applied to characterize the synthesized product. Moreover, the influences of ultrasonic irradiation including temperature, time, and power on different features of the final products were systematically studied using 2{sup k-1} factorial design experiments, and the response surface optimization was used for determining the best welding parameter combination. The results obtained from analyses of variances showed that ultrasonic parameters affected the size distribution, thermal behaviour, and surface area of Ta-MOF samples. Based on response surface methodology, Ta-MOF could be obtained with mean diameter of 55 nm, thermal stability of 228 °C, and high surface area of 2100 m{sup 2}/g. The results revealed that the synthesized products could be utilized in various applications such as a novel candidate for CO{sub 2} adsorption. - Graphical abstract: A facile route was used for fabrication of a new metal -organic framework based on tantalum nanostructures that have high surface area, considerable porosity, homogenous morphology, and small size distribution.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Phase transition and negative thermal expansion of HfMnMo3O12

Highlights: • HfMnMo{sub 3}O{sub 12} exhibits negative thermal expansion from 373 K to 773 K. • The linear CTE of HfMnMo{sub 3}O{sub 12} is −3.8 × 10{sup −6} K{sup −1}. • Vibrational modes corresponding to librational and translational motions of the polyhedra are observed. - Abstract: A novel compound HfMnMo{sub 3}O{sub 12} with negative thermal expansion (NTE) was synthesized using solid state method. The crystal structure, fracture morphology and NTE properties of the material were investigated by temperature-dependent X-ray diffraction (XRD), scanning electron microscope (SEM) and temperature-dependent Raman spectra. Our experimental results show that the compound adopts a monoclinic symmetry below room temperature and transforms to an orthorhombic phase above 348 K. In the orthorhombic phase the compound exhibits NTE property with a linear coefficient of thermal expansion (CTE) −3.8 × 10{sup −6} K{sup −1} from 400 K to 700 K. The physical mechanism of the NTE is discussed and elucidated according to our experiments.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

AC Susceptibility and Superconducting Properties of Graphene Added YBa{sub 2}Cu{sub 3}O{sub 7−d}

The effect of graphene (G) addition on YBa{sub 2}Cu{sub 3}O{sub 7−δ}(G){sub x} (x = 0 − 0.03 wt%) has been studied using the X-ray diffraction method, scanning electron microscopy, electrical resistance versus temperature, transport critical current density J{sub c}, and AC susceptibility measurements. XRD patterns showed single-phase YBa{sub 2}Cu{sub 3}O{sub 7−δ} (YBCO) for all samples. SEM micrographs showed filling of the voids between YBa{sub 2}Cu{sub 3}O{sub 7−δ} grains as graphene was added. The temperature-dependent electrical resistance curves showed metallic normal state behavior and onset transition temperature T{sub conset} between 90 and 92 K for all samples. AC susceptibility measurement showed transition temperature T{sub cχ{sup ′}} between 90 and 93 K. T{sub cχ{sup ′}} was maintained or improved slightly as graphene was added. The x = 0.001 wt% showed the highest J{sub c}, i.e., 2750 A cm{sup −2} at 77 K and 5570 mA cm{sup −2} at 30 K which was 13 and 40 times higher than that of the non-added YBCO, respectively. The peak temperature T{sub p} of the imaginary part of the susceptibility χ{sup ″} was around 78–82 K for all samples indicating grain coupling was not weakened as graphene was added.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Magnetic Performance and Evaluation of Radiofrequency Hyperthermia of Perovskite La{sub 1−x}Sr{sub x}MnO{sub 3}

Magnetic nanoparticles (MNPs) can induce localized hyperthermia by alternating magnetic fields, in order to kill cells at tumor sites. In this study, La{sub 1−x}Sr{sub x}MnO{sub 3} nanoparticles with x = 0.2, 0.3, 0.4, and 0.5 were prepared via sol–gel technique. The synthesized nanoparticles were characterized in terms of structure, morphology, and magnetic properties with Fourier transform infrared (FTIR), X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), and vibrating sample magnetometer (VSM) studies. The average size of nanoparticles was measured to be 57.09, 30.477, 10.24, and 35.982 nm by Williamson–Hall method for x = 0.2, 0.3, 0.4, and 0.5, respectively. The absence of hysteresis in the magnetic response of nanoparticles represents the superparamagnetic behavior. Toxicity test was also performed to evaluate the toxicity concerns of the prepared nanoparticles upon entrance to the body. Furthermore, the alternating current magnetic heating characteristics of La{sub 1−x}Sr{sub x}MnO{sub 3} nanoparticles was also studied, by 1 mg/mL concentration, to test the ability of the nanoparticles as magnetic hyperthermia treatment agents. The magnetothermia were measured in an RF magnetic field of 88 Oe and 430 kHz. The present work reveals that LSMO nanoparticles possess the biocompatible properties for biomedical applications and can provide the required heat at appropriate time.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Effect of SiO{sub 2} on the Formation of Acicular Calcium Ferrite in Sinter

SiO{sub 2} greatly influences the formation of acicular calcium ferrite (ACF), which is the main binder phase in sinter, but the mechanism of its influence is not yet clear. Experiments were carried out under air at 1200 °C with different amounts of SiO{sub 2} mixed with Fe{sub 2}O{sub 3} and Ca(OH){sub 2}. X-ray diffraction (XRD), scanning electron microscopy (SEM), energy-dispersive spectroscopy (EDS), and three-dimensional (3D) reconstruction were used to characterize the phase and morphological changes of the sintered samples. The results show that SiO{sub 2} can form silicon-ferrite of calcium (SFC), which is beneficial to the formation of ACF in sinter. The SFC content first increased and then decreased with the increasing SiO{sub 2} content. The sintered sample contained the highest contents of SFC and ACF when w(SiO{sub 2}) was 3 to 4 pct. The morphological changes in calcium ferrite observed with the increasing SiO{sub 2} content followed a sequence of massive → platy → acicular; both platy calcium ferrite and ACF were the longest in one direction in their 3D morphology. The inclusion of Si{sup 4+} in calcium ferrite crystals changes the crystal growth habit from having no obvious orientation to having a preferential orientation along the (040) or (320) surfaces, as determined by the first-principles calculations and XRD analysis of block samples. Viscosity was the main environmental factor influencing the size of ACF in samples with sufficient liquid phase.

36 MATERIALS SCIENCE↗

Characterisation of organic-inorganic hybrid materials of the types ZnxCd1-xSe(1,3-diaminopropane)1/2 and ZnSySe1-y(1,3-diaminopropane)1/2

Highlights: • New hybrid materials: Zn{sub x}Cd{sub 1-x}Se(1,3-DAP){sub 1/2} and ZnS{sub x}Se{sub 1-x}(1,3-DAP){sub 1/2} were obtained. • Hybrids were studied using XRD, TG/DSC, XRD vs. temperature, SEM, UV–vis spectroscopy. • The impact of the composition of the layers on optical properties were studied. - Abstract: Organic-inorganic hybrid materials of the type MeQ(diamine){sub 1/2} (where Me–Zn, Cd, Mn and Q–S, Se, Te) belong to the class of 3D nanomaterials. They are built of layers of II–VI semiconductors and amines, which act as linkers. The main goal of our work was the synthesis of compounds of the type Zn{sub x}Cd{sub 1-x}Se(1,3-diaminopropane){sub 1/2} and ZnS{sub y}Se{sub 1-y}(1,3-diaminopropane){sub 1/2} (where x, y = 0, 0.25, 0.5, 0.75, 1) and the study of properties changed by the composition of the semiconducting layers. Analysis of these materials was carried out with the use of X-ray powder diffraction (XRPD), scanning electron microscopy (SEM), simultaneous thermogravimetry and differential scanning calorimetry (TG-DSC) as well as temperature dependent XRPD enabled us to obtain information about the thermal stability of hybrid compounds with mixed semiconducting layers. Another important part of our work was a study, performed with the use of UV–vis spectroscopy, of the optical properties of these materials.

77 NANOSCIENCE AND NANOTECHNOLOGY↗

Growth and properties of crystalline CuInSe{sub 2} thin films by SPD technique

CuInSe{sub 2} thin films were grown on glass substrates using the chemical spray pyrolysis technique. The CuInSe{sub 2} films were co-deposited from aqueous solutions containing CuCl{sub 2}, InCl{sub 3}, and SeO{sub 2} used as Cu, In and Se precursors respectively. EDC was used as a complexing agent and films were grown at the constant temperature of 270°C. The films were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM) and Energy dispersive analysis of X-rays (EDAX) and the results indicate that the films are single phase, p-type in conductivity and have the chalcopyrite structure. Optical study shows that the optical band gap value is 1.03 eV. From the XRD study it is clear that the average crystallite size of the films is in the range 50 to 70 nm.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Structural and Magnetic Characteristics of Ferroxplana Co{sub 2}Y Nanoferrites Synthesized via Two Chemical Routes

Barium Y-type hexaferrite Ba{sub 2}Co{sub 2}Fe{sub 12}O{sub 22} nanopowders have been purposefully tailored using two different chemical wet methods, namely sol-gel auto-combustion (SGA) and co-precipitation (CP) routes. The impact of the pre-annealing and the annealing temperature of the formed precursors synthesized using two strategies on the structural, microstructure, and magnetic properties was investigated using x-ray diffraction (XRD), scanning electron microscopic (SEM), Fourier transform infrared spectroscopy (FT-IR), and vibrating sample magnetometer (VSM). For instance, well-defined Ba{sub 2}Co{sub 2}Fe{sub 12}O{sub 22} hexagonal plate-like particles was observed using SGA and CP routes for the precursors pre-annealed at 600 {sup ∘}C for 4 h and then annealed at low temperature 1000 {sup ∘}C for 2 h. The magnetic properties measured at room temperature evinced that hexaferrite Co{sub 2}Y particles have ferromagnetic characteristics. Good magnetic properties involving saturation magnetization (M{sub s}) of 23.64 and 24.37 emu/g and the coercivity (H{sub c}) of 417.76 and 280.92 Oe were accomplished for the samples pre-annealed at 600 {sup ∘}C for 4 h and then annealed at 1000 {sup ∘}C for 2 h for SGA and CP methods, respectively.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Electrical, Structural, and Thermal Properties of Ferrite/Superconductor (Ni{sub 0.5}Zn{sub 0.5}Fe{sub 2}O{sub 4}){sub x}/YBa{sub 2}Cu{sub 3}O{sub 7-δ}) Nanocomposite Materials

The superconductor YBa{sub 2}Cu{sub 3}O{sub 7-δ} (Y123) is prepared by the solid-state route, while the nanosized Ni{sub 0.5}Zn{sub 0.5}Fe{sub 2}O{sub 4} (Ni-Zn ferrite) is synthesized via citric acid sol-gel technique. The composite material of the type (Ni{sub 0.5}Zn{sub 0.5}Fe{sub 2}O{sub 4}){sub x}/YBa{sub 2}Cu{sub 3}O{sub 7-δ}, where x = 0.00, 0.03, 0.10, and 0.50 wt%, is prepared by a modified solid-state method to study the effect of doping Ni-Zn nanosized ferrite on the superconducting, structure, and thermal properties of Y123. The prepared samples show Meissner effect which confirmed the presence of superconducting phase at liquid nitrogen temperature (77 K). The prepared samples have been characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), energy dispersion of X-ray (EDX), infra-red (IR) spectroscopy, thermogravimetric analysis (TGA), vibrating sample magnetometer (VSM), DC resistance by four-probe, and critical current density measurements. It was found that by increasing Ni{sub 0.5}Zn{sub 0.5}Fe{sub 2}O{sub 4} nanoparticles in the Y123 compound, the unit cell volume of the orthorhombic phase decreases, but the transition temperature T{sub c} and critical current density J{sub c} decrease for low doping (x = 0.03 wt%) then increase (x = 0.10 and 0.50 wt%) for Ni{sub 0.5}Zn{sub 0.5}Fe{sub 2}O{sub 4} doped in Y123. The transport properties of the (Ni{sub 0.5}Zn{sub 0.5}Fe{sub 2}O{sub 4}){sub x}/YBa{sub 2}Cu{sub 3}O{sub 7}-{sub δ} composite as electrical resistance R, T{sub c}, and J{sub c} are interpreted according to Bean’s critical state model and charge-vortex interaction combined with vortex pinning in Y123 high-T{sub c} mixed-state type-II superconductor. Highlights: The critical current density J{sub c} decreased for low doping of nanosized Ni-Zn ferrite into Y123 with ratio of 0.03 wt% and increased by increasing doping ratio to 0.50 wt%. The physical properties are improved by the coexistence of the superconductor Y123 and nanosized Ni-Zn ferrites in nanocomposite material.

77 NANOSCIENCE AND NANOTECHNOLOGY↗

Analysis of Al diffusion processes in TiN barrier layers for the application in silicon solar cell metallization

An evaporated Al layer is known as an excellent rear metallization for highly efficient solar cells, but suffers from incompatibility with a common solder process. To enable solar cell-interconnection and module integration, in this work the Al layer is complemented with a solder stack of TiN/Ti/Ag or TiN/NiV/Ag, in which the TiN layer acts as an Al diffusion barrier. X-ray photoelectron spectroscopy measurements prove that diffusion of Al through the stack and the formation of an Al{sub 2}O{sub 3} layer on the stack's surface are responsible for a loss of solderability after a strong post-metallization anneal, which is often mandatory to improve contact resistance and passivation quality. An optimization of the reactive TiN sputter process results in a densification of the TiN layer, which improves its barrier quality against Al diffusion. However, measurements with X-ray diffraction and scanning electron microscopy show that small grains with vertical grain boundaries persist, which still offer fast diffusion paths. Therefore, the concept of stuffing is introduced. By incorporating oxygen into the grain boundaries of the sputtered TiN layer, Al diffusion is strongly reduced as confirmed by secondary ion mass spectroscopy profiles. A quantitative analysis reveals a one order of magnitude lower Al diffusion coefficient for stuffed TiN layers. This metallization system maintains its solderability even after strong post-metallization annealing at 425 °C for 15 min. This paper thus presents an industrially feasible, conventionally solderable, and long-term stable metallization scheme for highly efficient silicon solar cells.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Mechanism of Texture and Precipitates Evolution in CGO Silicon Steel During High-Temperature Annealing Process

Grain-oriented silicon steel is an important soft magnetic material for electrical applications. A conventional grain-oriented silicon steel with final thicknesses of 0.27, 0.23 and 0.20 mm was prepared separately by a two-stage cold rolling process. Texture evolution, precipitates distribution and Goss textures formed during secondary recrystallization were analyzed by electron backscattered diffraction and field emission scanning electron microscopy. The results show that plate thickness influences the distribution density of secondary phase particles and the content of favorable texture components such as {111} <112>, {111} <110> and {112} <110> texture. Decreasing plate thickness increases the areal density of secondary phase particles, the temperature of secondary recrystallization, which also increases the content of favorable texture component, and the strength of Goss texture in secondary recrystallization. Goss grains have higher particle density than the grains with other orientations, which facilitates their abnormal growth by swallowing surrounding grains with lower particle density.

36 MATERIALS SCIENCE↗

One-pot synthesis of Ni/Ni{sub 3}C/Ni{sub 3}N nanocomposite: Structure, growth mechanism and magnetic properties

Graphical abstract: Ni/Ni{sub 3}C/Ni{sub 3}N nanocomposites were synthesized by a one-pot solution chemistry method at lower temperature of 200 °C. The formation mechanism, magnetic properties and textural structures of Ni/Ni{sub 3}C/Ni{sub 3}N nanocomposite were investigated. - Highlights: • Ni/Ni{sub 3}C/Ni{sub 3}N nanocomposites were synthesized by a one-pot solution chemistry method at lower temperature of 200 °C. • Ni{sub 3}N nanomaterials were generally obtained by two steps, here we use one-step for preparation of Ni{sub 3}N nanomaterials. • The formation mechanism, magnetic properties and textural structures of Ni/Ni{sub 3}C/Ni{sub 3}N nanocomposite were investigated. - Abstract: A one-pot solvothermal synthesis of Ni/Ni{sub 3}C/Ni{sub 3}N nanocomposite, using hydrazine hydrate (N{sub 2}H{sub 4}) as reducing agent and tetraethylene glycol (TEG) as solvent, is reported. The contents of Ni{sub 3}C and Ni{sub 3}N decrease with increasing the amount of N{sub 2}H{sub 4}. The magnetic hysteresis loops at room temperature of the Ni/Ni{sub 3}C/Ni{sub 3}N display ferromagnetic characteristics. Saturation magnetization increases gradually with increasing Ni content of the Ni/Ni{sub 3}C/Ni{sub 3}N. Growth mechanism is discussed based on the characterization results of X-ray diffraction (XRD), scanning electron microscope (SEM), and X-ray photoelectron spectroscopy (XPS), thermogravimetric analysis (TG), nitrogen adsorption desorption, and elemental analysis. Furthermore, Ni{sub 3}N was fabricated by such a solution chemistry method at low-temperature of 200 °C.

36 MATERIALS SCIENCE↗