Elsevier

Journal of Alloys and Compounds

Volume 605, 25 August 2014, Pages 230-236
Journal of Alloys and Compounds

Optimal synthesis and magnetic properties of size-controlled nickel phosphide nanoparticles

https://doi.org/10.1016/j.jallcom.2014.03.110Get rights and content

Highlights

  • A pulse discharge method was used to synthesize noncrystalline Ni-P nanoparticles.

  • Size controlled nanoparticles were prepared through adjustment of reaction parameters.

  • Local structures both centered around Ni and P atoms were investigated including coordinated atoms and bondlengths.

  • Magnetic properties of the nickel phosphide nanoparticles are found to be ferromagnetic and size-dependent.

Abstract

Pulse discharge method was used in liquid phase to prepare nickel phosphide nanoparticles. The size and morphology of the as-prepared nanoparticles were found to be easily controlled through changing reaction parameters such as temperature, reactants concentration, reactants molar ratio, pulse discharge number, and pulse discharge voltage. The optimal reaction parameters have been obtained by single-factor experiments. X-ray diffraction, X-ray absorption fine structure spectra, Field Emission Scanning Electron Microscope, and Energy Dispersive X-ray Spectrum were used to characterize the as-prepared Ni–P nanoparticles. Vibrating Sample Magnetometer was used as magnetic measurements of the Ni–P nanoparticles. The results demonstrate that the as-prepared Ni–P nanoparticles are in amorphous phase, and consist of Ni and P elements. The P-content in the as-prepared Ni–P nanoparticles increases with the increasing of Ni–P particle size, and is independent on the initial concentration of P-concentration in the reaction solution. The Ni–P nanoparticles have totally about 12 near-neighbors of Ni–Ni and Ni–P around center Ni. The Ni–Ni distance increases with the increasing particle size. The as-prepared Ni–P nanoparticles present paramagnetic nature. Their saturated magnetizations are also size-dependent. The larger Ni–P particles has lower saturated magnetization, which can be attributed to the entrance of P into Ni lattice, causing a larger Ni–Ni separation and a looser, distorted local atomic structure.

Introduction

Nickel phosphides are a class of compounds that have properties similar to those of ordinary metallic compounds such as carbides, nitrides, borides and silicides. They are good conductors of heat and electricity and they have high thermal and chemical stability. Due to their properties of fundamental and commercial interest, transition metal phosphides have been used as excellent catalysts for hydrodesulfurization (HDS) and hydrodenitrogenation (HDN) [1], electrocatalysts for hydrogen evolution reaction (HER) [2], magnetic storage for their magnetic properties [3], and electrode materials for Li batteries [4], [5]. Therefore, the synthesis of nickel phosphides has attracted extensive attention since several decades. Multiple synthesis routes, for example, the solid phase reaction [6], the solution-phase reaction [7], [8], [9], [10], the decomposition of single source precursors [11], the thermolysis of nickel compounds [12], and relatively inexpensive synthesis method [13], have been reported for the preparation of nickel phosphides with different shapes (solid particles, core–shell particles, rods, and wires) in recent years. Synthesis methods of amorphous nickel phosphide nanoparticles have also been developed [14], [15]. However, the report about size-controllable synthesis of Ni–P nanoparticles is scarce. Little is known about their local ordering and the implications of their structure on their novel properties due to the limitation of X-ray diffraction (XRD) and transmission electron microscope (TEM) techniques [16].

Although techniques that enable the structure characterization of bulk material have been well-developed, the characterization of material at the nanoscale still presents significant challenges. The dominance of surface facets, small size and poor crystalline order makes characterization of nanoparticles difficult. X-ray absorption spectroscopy (XAS) is a method that has been used to resolve the structure of colloidal nanocrystals. With the use of the X-ray beam available through synchrotron radiation facility, XAS spectra can be obtained and used to gain insight into material structural properties [17], [18]. The structures of amorphous and crystalline phases can be determined through both X-ray-absorption near-edge-structure (XANES) spectrum to resolve geometric configuration, and extended X-ray-absorption fine-structure (EXAFS) to resolve radial structure, including interatomic distances, coordination numbers, and mean-squared disorder [19].

In this paper, a size-controllable preparation of nickel phosphide nanoparticles was performed through pulse discharge method. Reaction conditions such as temperature, solution concentration, reactants molar ratio, pulse number and pulse voltage were adjusted to obtain nanoparticles with different size distributions. Field Emission Scanning Electron Microscope (FESEM) pictures and Energy Dispersive X-ray Spectrum (EDS) spectra were collected through traditional laboratory experiments to determine morphology and composition of the as-prepared nanoparticles. XRD patterns and X-ray-absorption fine-structure (XAFS) spectra from both Ni K-edge and P K-edge were collected at Beijing Synchrotron Radiation Facility (BSRF) to resolve phase and atomic ordering. Size-dependent magnetic property was also measured through Vibrating Sample Magnetometer (VSM).

Section snippets

Preparation of samples

A pulsed-discharge method was used to prepare the Ni–P nanoparticles. The pulse discharge generator is home-made with a peak voltage of 1200 V and a peak current of 6 A. The schematic map of this one-step pulsed-discharge appliance is described in Fig. 1. Two commercially available reagents, i.e. nickel–sulfate hexahydrate (NiSO4·6H2O) and sodium hypophosphite (NaH2PO2·H2O), were directly used as the raw materials without further purification. The preparation detail of the reaction solution is

Effects of reaction parameters on particle size distribution and morphology

In order to control the particle size of the as-prepared Ni–P nanoparticles, five groups of single-factor experiment were carried out under different temperatures, reactant concentrations, reactant ratios, pulse numbers and pulse voltages. Each impact of the five reaction parameters on the size-distribution and morphology of Ni–P nanoparticles were investigated. In these experiments, only one of the reaction parameters was variable at each time, while the others were kept constant. The detailed

Conclusion

Nickel phosphide nanoparticles were prepared through liquid pulse discharge method. The effect of reaction parameters on particle-size distribution and morphology of the as-prepared Ni–P nanoparticles has been studied. Generally, higher temperature and solution concentration are in favor of small particles, while the reactants molar ratio, pulse discharge number and pulse discharge voltage have optimal values for the synthesis of uniform Ni–P nanoparticles. Single-factor experiments were

Acknowledgement

This work was supported by National Natural Science Foundation (Nos. 51374019, U1232203, 10385008, 50374010) of China.

References (28)

  • G. Shi et al.

    New synthesis method for nickel phosphide nanoparticles: solid phase reaction of nickel cations with hypophosphites

    J. Mater. Chem.

    (2009)
  • M. Elayaraja et al.

    Synthetic levers enabling independent control of phase, size, and morphology in nickel phosphide nanoparticles

    ACS Nano

    (2011)
  • X. Zheng et al.

    Nickel/nickel phosphide core-shell structured nanoparticles: synthesis, chemical, and magnetic architecture

    Chem. Mater.

    (2009)
  • W. Maneeprakorn et al.

    Synthesis of the nickel selenophosphinates [Ni(Se2PR2)2] (R = iPr, tBu and Ph) and their use as single source precursors for the deposition of nickel phosphide or nickel selenide nanoparticles

    J. Dalton Trans.

    (2009)
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