I. INTRODUCTION
Many mixed oxides of the type A 2BO4 (A = rare earth, alkaline earth; B = transition metal) crystallize with the K2NiF4-type structure that can be described as an ordered intergrowth alternating perovskite (ABO3) and rock salt (AO) layers. The BO6 octahedra shares corners, forming a two-dimensional array of B–O–B bonds which is responsible for a variety of interesting physical phenomena, such as, the anisotropic electrical transport and magnetic exchange interactions (Bassat et al., Reference Bassat, Odier and Gervais1987; Buttrey and Honig, Reference Buttrey and Honig1988). Rare earth nickelates show a considerable range of oxygen non-stoichiometry depending on their synthetic preparations (Arbuckle et al., Reference Arbuckle, Ramanujachary, Zhang and Greenblatt1990). The excess of oxygen is attributed to intergrowth of Ruddelsden–Popper-type phases (Odier et al., Reference Odier, Nigara and Coutures1985), variable valence of the transition metal ion and more recently to the incorporation of interstitial oxygen defects (Jorgensen et al., Reference Jorgensen, Dabrowski, Pei, Richards and Hinks1989). The structural and magnetic properties of Ln2NiO4+δ-type compounds were reported to be extremely sensitive to the deviations in the oxygen stoichiometry (Buttrey et al., Reference Buttrey, Honig and Rao1986; Buttrey and Honig, Reference Buttrey and Honig1988; Rodriguez-Carvajal et al., Reference Rodriguez-Carvajal, Martinez and Pannetier1988; Demourgues et al., Reference Demourgues, Wattiaux, Grenier, Pouchard, Soubeyroux, Dance and Hagenmuller1993).
It was reported that Nd2NiO4+δ can have either monoclinic or orthorhombic symmetry. The source of the structural difference is unclear; it may be because of the oxygen content or structural defects (Arbuckle et al., Reference Arbuckle, Ramanujachary, Zhang and Greenblatt1990). It was also reported that NdSrNiO4 has tetragonal symmetry (Takeda et al., Reference Takeda, Nishijima, Imanishi, Kanno, Yamamoto and Takano1992). It was thought that the substitution of Nd by Sr in Nd2NiO4+δ might induce a structural phase transition from orthorhombic to tetragonal symmetry leading to a mixed valence for the transition metal ion, which would in turn induce interesting electrical and magnetic properties in this system.
The layered K2NiF4-type Ln2−xSrxNiO4−δ solid solutions for Ln = La, Nd, Pr, Sm and Gd have been extensively studied (Gopalakrishnan et al., Reference Gopalakrishnan, Colsmann and Reuter1977; Arbuckle et al., Reference Arbuckle, Ramanujachary, Zhang and Greenblatt1990; Sreedhar and Rao, Reference Sreedhar and Rao1990; Takeda et al., Reference Takeda, Kanno, Sakano, Yamamoto, Takano, Bando, Akinaga, Takita and Goodenough1990, Reference Takeda, Nishijima, Imanishi, Kanno, Yamamoto and Takano1992; Chen et al., Reference Chen, Cheong and Cooper1993). A unique set of these properties makes them useful as electrode materials in different electrochemical devices. Further investigations into these oxides have been carried out to find appropriate compositions with the best set of necessary properties.
Takeda et al. (Reference Takeda, Nishijima, Imanishi, Kanno, Yamamoto and Takano1992) investigated the structural and physical properties of the Nd2−xA xNiO4 systems (A = Ca, Sr, or Ba). The solid solution limits of alkaline earth were 0.6, 1.4 and 0.6 for Ca, Sr and Ba, respectively. In spite of the substitution of different alkaline earth metals, the distances of Ni–O showed no dependence with this action. The effect of this substitution was reflected on the Nd/Ca–O and Nd/Ba–O distances along the c-axis. The neodymium alkaline earth nickelates, therefore give good insights into the evolution of the perovskite structure owing to the deformation of the A site, resulting from the above-mentioned substitution. All Nd2−xCaxNiO4 samples have the orthorhombic (Bmab and Fmmm) structure. For Nd2−xSrxNiO4 and Nd2−xBaxNiO4, there were tetragonal I4/mmm phases. A semiconductor–metal transition was observed for 0 < x < 1.0 in Nd2−xSrxNiO4 systems, the transition temperature decreased from 450 K (x = 0. 1) to 100 K (x = 1.0), but it exhibited a change in characteristic at x = 0.6.
In our previous works we successfully prepared neodymium NdSrNi1−xCuxO4−δ 0 ≤ x ≤ 1 and studied their structural and electrical properties (Chaker et al., Reference Chaker, Roisnel, Potel and Ben Hassen2004, Reference Chaker, Roisnel, Cador, Amami and Ben Hassen2006). After that an investigation into the quaternary Ln2O3–SrO–NiO-CuO system showed a similar structure for LnSr5Ni2.4Cu0.6O12−δ with the smaller lanthanides cations Dy, Ho and Er (Chaker et al., Reference Chaker, Roisnel, Ceretti and Ben Hassen2007; Hamdi et al., Reference Hamdi, Ouni, Chaker, Rohlicek and Ben Hassen2011).
Tonus et al. (Reference Tonus, Bahout, Battle, Hansen, Henry and Roisnel2010) recently introduced a combination of nickel and chromium into the K2NiF4 structure by synthesizing Ln3−xSr1+xNiCrO8−δ (Ln = La, Nd) with the aim of identifying potential anode materials for Solid Oxide Fuel Cells (SOFCs). Their approach of selecting Cr/Ni-based compositions was influenced by the relative success of the analogous perovskite system. This stems firstly from the stability of Cr3+ to hydrogen reduction and the structural stability that this confers. Secondly, it relies on the electrocatalytic properties of the Ni cation and its ability to lower its oxidation state and coordination number to generate the oxygen-vacancy network needed for anionic conduction.
As, we are much more interested in mixed oxides based on neodymium, we have recently studied the series NdSrNi1−xCrxO4+δ, 0 ≤ x ≤ 1 (Jammali et al., Reference Jammali, Chaker, Cherif and Ben Hassen2010) and the transport mechanism in this series was investigated. Our results found that these compounds exhibit a poor semi-conductive behaviour.
The aim of this work is to investigate the effect of chromium incorporation on the structural and physical properties of Nd2−xBaxNiO4+δ, systems with a bigger amount of alkaline earth which have not yet been reported. In this work, we report the results of powder X-ray diffraction (XRD) analysis, oxygen-content determination and electrical measurements of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ.
II. EXPERIMENTAL
A. Synthesis
The Nd1.7Ba0.3Ni0.9Cr0.1O4+δ sample was prepared in polycrystalline form by sol–gel route. Stoichiometric quantities of Nd2O3 (Aldrich 99.99%), pre-dried in air at 1223 K to remove any hydrogeno-carbonate impurities, BaCl2 · 2H2O (Aldrich 99.99%), Cr(NO3)3 · 9H2O (Aldrich 99.99%) and NiO (Aldrich 99.99%), as appropriate, were dissolved in a minimum quantity, typically 150 ml, of a 1:1 solution of analaR 6-M nitric acid and distilled water. For each mole of transition metal, 3-mol equivalents of citric acid (C6H8O7, 98%) solution were added along with 5 ml of ethylene glycol. The stirred solution was heated on a hot plate and the liquid evaporated gradually. A gel was formed and then dehydrated on a hot plate until a black powder residue remained. This residue was ground and calcined in a furnace at 1073 K for 12 h to remove the remaining organic component. The resultant powder was subsequently ground and heated in argon at 1523 K for 96 h. In between the sintering steps, the sample was cooled and then grounded.
B. Data collection and electrical measurements
Powder XRD pattern of the new compound was collected at room temperature using a Diffractometer Empyrean of PANalytical equipped with an incident-beam curved Ge (111) Johansson monochromator to obtain Cu Kα 1 radiation (λ = 1.54056 Å). Data were collected at each 0.007° step width, for 50 s over a 2θ range from 10.003 to 150.017°, and a PIXcel3D solid-state X-ray detector was used in the Bragg–Brentano geometry.
Direct current resistivity measurements were carried out on sintered pellets using a Lucas Labs 302 four-point probe with a Keithley 2400 digital Source Meter (Keithley Instruments Inc., Cleveland, Ohio). Measurements were performed in the temperature range between 313 and 708 K.
The oxygen content of the single-phase powder was indirectly determined at room temperature after calculation of the valence average of the transition metal ions obtained by iodometric titration. In fact, about 50 mg of the sample were dissolved in a solution of 6-M hydrochloric acid in the presence of excess KI, leading to reduction of tri- and tetra-metal transition ions and formation of iodine that was titrated with Na2S2O3 solution using starch as indicator. The sodium thiosulfate solution was standardized using pure copper wire.
III. RESULTS AND DISCUSSION
A. Crystal structure and oxygen content
The purity of the prepared sample was confirmed by laboratory powder XRD measurements, which revealed neither impurities nor starting materials.
The most intense observed lines in the pattern of the new phase were selected to establish the procedure of indexing by means of DICVOL91 program (Boultif and Lauër, Reference Boultif and Louër1991). It was found that Nd1.7Ba0.3Ni0.9Cr0.1O4+δ adopts the tetragonal K2NiF4-type structure with I4/mmm space group. The refined unit-cell parameters are listed in Table I.
Crystal data for Nd1.7Ba0.3Cr0.1Ni0.9O4+δ.
The Rietveld refinement was carried out with the pseudo-Voigt function used for the simulation of peak shapes. First, we started with refinement of the zero-point instrument, unit-cell parameters, half-width parameters U, V, W and then, the background was fitted with a linear interpolation between 99 chosen points. The structural refinement was carried out in the space group I4/mmm with Nd/Ba and O(2) atoms [situated at special positions 4e with coordinates (0, 0, z)]. The Ni and Cr atoms are located at (0, 0, 0) in the 2a site and the O(1) atoms at (0, ½, 0) in the 4c site. Atomic positions have been refined for all the atoms, together with the scale factor and profile parameters. The refinements of all isotropic temperature factors including those of oxygen were stable, and the least square analysis converged quickly to provide a good fit to the diffraction pattern.
It was impossible to refine the Ni/Cr ratio, owing to the similar X-ray scattering powers of these elements. The refinements of the isotropic temperature factors were unstable, but good results were obtained by refinement of overall isotropic displacement factor. Finally, refinement of the preferred orientation correction in the [001]-direction led to a highly significant diminution of χ 2, and a considerable improvement in the quality of the fit. A final refinement converged to R B = 4.37%, R wp = 12.2% and χ 2 = 3.00, R p = 15.2% and R F = 4.38%. The Rietveld refinement procedures were used with the help of the FULLPROF software (Rodríguez-Carvajal, Reference Rodriguez-Carvajal1990).
The stability of the Nd1.7Ba0.3Ni0.9Cr0.1O4+δ compound having the K2NiF4-type structure can be discussed in terms of the value of the tolerance factor defined by Goldschmidt (Ganguly and Rao, Reference Ganguly and Rao1984) as
The K2NiF4-type structure is stable over the range 0.866 ≤ t < 1. The T (tetragonal) structure exists for 0.88 ≤ t ≤ 0.99 and the T/O (tetragonal/orthorhombic) structure is present for 0.866 ≤ t < 0.88. Based on Shannon's ionic radii (Shannon, Reference Shannon1976) (rNd3+ = 1.163 Å, r Ba2 + = 1.47 Å in a 9-fold coordination and rNi3+ = 0.56 Å, in the low-spin case, rCr3+ = 0.615 Å and rO2− = 1.4 Å in a 6-fold coordination), the theoretical tolerance factor for Nd1.7Ba0.3Ni0.9Cr0.1O4+δ is t = 0.938, this value was included in the tetragonal symmetry stability range. Consequently, refinement of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ X-ray data has been performed to confirm the K2NiF4-type structure.
To study the variation in the oxygen content, we carried out iodometric titration using Na2S2O3 standard solution. The oxygen non-stoichiometry (δ) is directly correlated to the Ni3+ and Cr4+ content according to the formulation Nd1.7Ba0.3(Ni3+1−τ Ni2+τ)0.9(Cr4+1−τ Cr3+τ)0.1O4+δ, with δ = (0.8 − τ)/2. The content (1 − τ) of the average of cation transition metals Ni3+ and Cr4+ was determined by iodometric titration. I− anions reduce dNi3+ cations into Ni2+ and reduce Cr4+ cations into Cr3+. The titration of the resulting I2, by a solution of Na2S2O3 sodium thiosulfate led, by considering the average of cations transition metals Ni3+ and Cr4+, to the value τ = 0.67 and therefore δ = 0.06, indicating excess oxygen in the sample.
B. Structure description
The observed, calculated and difference profiles for the Rietveld refinement of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ compound are shown in Figure 1. The structurally refined parameters for Nd1.7Ba0.3Ni0.9Cr0.1O4+δ are summarized in Table II.
The observed, calculated and difference profiles for the Rietveld refinement of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ compound.
Structural parameters of Nd1.7Ba0.3Cr0.1Ni0.9O4+δ obtained from Rietveld refinements of powder XRD data.
As shown in Figure 2, the structure of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ sample can be described as an ordered intergrowth of alternating perovskite (Nd/Ba)(Ni/Cr)O3 and rock salt (Nd/Ba)O layers stacked along the tetragonal c-axis. The (Ni/Cr)O6 octahedra shares corners in the ab-plane forming a two-dimensional array of (Ni/Cr)-O-(Ni/Cr) bonds, which is responsible for a variety of interesting physical phenomena, such as, the anisotropic electrical transport and magnetic exchange interactions (Bassat et al., Reference Bassat, Odier and Gervais1987; Buttrey and Honig, Reference Buttrey and Honig1988).
Crystal structure of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ sample with the tetragonal K2NiF4-type structure.
The neodymium and barium atoms are surrounded by nine oxygen atoms (Figure 2). By examining the nine (Nd/Ba)–O bonds, it should be noted that all of them present distances lying between 2.2837 and 2.7440 Å slightly lower than the sum of the ionic radii of Ba2+ (R Ba2+ = 1.47 Å) and O2− (R O2− = 1.42 Å) given by Shannon (Reference Shannon1976). This result confirms the prevalence of the covalent character of these bonds. The interatomic distances and bond angles for Nd1.7Ba0.3Ni0.9Cr0.1O4+δ compound are listed in Table III.
The interatomic distances and bond angles for Nd1.7Ba0.3Ni0.9Cr0.1O4+δ.
The prominent feature of perovskite structures is their flexibility with respect to relative cation size. This is generally achieved by tilting of the BX6 octahedral centre, leading to slight distortions of the octahedra (Elcombe et al., Reference Elcombe, Kisi, Hawkins, White, Goadman and Matheson1991). The (Ni/Cr)–O6 octahedra are untilted for the present structure model of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ, compared with Nd1.7Ba0.3NiO4+δ (Takeda et al., Reference Takeda, Nishijima, Imanishi, Kanno, Yamamoto and Takano1992). Thus, the distances (Ni/Cr)-O: d(Ni/Cr)-Oapical = 2.2081 Å and d(Ni/Cr)-Oplanar = 1.9125 Å are very close to Nd1.7Ba0.3NiO4+δ [(Ni/Cr)-Oapical = 2.20 Å and d(Ni/Cr)-Oplanar = 1.91 Å]. By substituting Ni with Cr, we assist in little changes in the unit-cell parameters that may mainly result from the small differences in ionic size of Ni3+/Ni2+ and Cr3+/Cr4+.
C. Electrical conductivity
To obtain dense ceramic pellets for electrical measurements, powder sample of the material was grounded (in ethanol). A pellet (13 mm in diameter and 1.8 mm thick) was prepared by uniaxial pressing (100 MPa). It was then sintered at 1373 K for 2 h to obtain a disc with high density. The total electrical conductivity σ of sintered ceramic was determined under air using the four-probe technique in the temperature range between 313 and 708 K.
The crystal structure of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ is made up of alternating rock-salt (Nd/Ba)2O2 and perovskite Ni/CrO2 layers, and can accommodate a significant oxygen excess. The extra O2− anions occupy interstitial positions in the (Nd/Ba)O bilayers. The equilibrium oxygen hyperstoichiometry (δ) in air is close to 0.06 at 300 K. The excess negative charge introduced by excess oxygen is neutralized by oxidation of Ni/Cr ions. As a result, the introduction of excess oxygen in the (Nd/Ba)O bilayers creates mobile holes in Ni/CrO6 octahedra. The increase in electrical conductivity with temperature can be explained by the increasing mobility of oxygen interstitials and holes.
The corresponding curve to σ vs. T is reported in Figure 3. The conductivity, increases with temperature in the whole range of temperature.
Thermal variation of the electric conductivity σ for the Nd1.7Ba0.3Ni0.9Cr0.1O4+δ compound (313 K ≤ T ≤ 708 K).
Figure 4 shows the relationship of ln (σT) vs. 1000/T for temperature range of 313–708 K. The increase in ln (σT) with increasing temperature indicates that the sample has semi-conductive behaviour at high temperature. To determine the conduction mechanism, we tried to use the thermally activated adiabatic small polaron hopping as the conduction model:
where E a is the activation energy (polaron formation and hopping energy), σ 0 is a constant related to polaron concentration and diffusion. In the analysis of simulated curve: ln(σT) = f(1000/T), we found that the convergence of the curve fitting was achieved in the whole range of temperature. This result implies that the transport properties in Nd1.7Ba0.3Ni0.9Cr0.1O4+δ, and in the temperature range of 313–708 K, are well described by the adiabatic small polaron hopping mechanism, where activation energy, after fitting, is E a = 0.013 eV.
Arrhenius relations of Ln(σT) vs. 1000/T for the Nd1.7Ba0.3Ni0.9Cr0.1O4+δ. The solid lines are the fitting curves of equation, and the points represent the experimental values.
By comparing the transport properties at high temperature between Nd1.7Ba0.3Ni0.9Cr0.1O4+δ and Nd1.7Ba0.3NiO4+δ samples, one can conclude that both samples show a semi-conductive behaviour, and partial substitution of the Ni by Cr decreases significantly the conductivity. Taking into account that both compounds have the same amount of oxygen hyperstoichiometry (δ), we can conclude that the mobility of oxygen interstitials remains unchanged, consequently holes concentration is reduced. This behaviour, contrary to the Nd2−xBaxNiO4+δ cases (Takeda et al., Reference Takeda, Nishijima, Imanishi, Kanno, Yamamoto and Takano1992), may suggest an important role of hole trapping by the chrome cations forming stable Cr3+ states. Such hypothesis seems well supported by numerous experimental data on the oxygen non-stoichiometry and phase stability of various LaSrCrO4-, LaSrNiO4-, LaSrCrO3- and LaSrNiO3-based solid solutions, which suggest a considerably higher stability of Cr3+ compared to Ni3+ (Sauvet and Irvine, Reference Sauvet and Irvine2004; Millburn and Rosseinsky, Reference Millburn and Rosseinsky1997).
IV. CONCLUSION
Nd1.7Ba0.3Ni0.9Cr0.1O4+δ compound was formed by sol–gel route and annealing at 1523 K in argon atmosphere. Rietveld refinement using powder XRD data shows that the title compound crystallizes in the tetragonal K2NiF4-type structure in space group I4/mmm. The results obtained by iodometric titration indicate excess oxygen in the sample. The investigation into the transport properties indicates that the electrical conductivity of Nd1.7Ba0.3Ni0.9Cr0.1O4+δ ceramic increased with increasing temperature. A semi-conductive behaviour is observed and the fitting shows that the adiabatic small polaron hopping model describes the experimental data in the temperature range between 313 and 708 K with an activation energy E a = 0.013 eV. By comparing the values of conductivities at high temperatures between Nd1.7Ba0.3NiO4+δ and Nd1.7Ba0.3Ni0.9Cr0.1O4+δ samples, it was concluded that the substitution of Ni by Cr significantly decreases the conductivity.
