Original Research PaperCharacterization and photocatalytic activity of Y-doped BiFeO3 ceramics prepared by solid-state reaction method
Graphical abstract
Introduction
Bismuth ferrite with a high Curie and Neel temperatures (TC ∼ 1103 K & TN ∼ 647 K) is the only well-known lead-free multiferroic material at and above room temperature (RT) [1], [2], [3], [4], [5]. Bulk BiFeO3 has distorted rhombohedral perovskite structure (with the space group of R3c) and G-type antiferromagnetic order [6], [7], [8]. BFO is widely used in data storage, spintronics, sensors and magneto-electric devices [9], [10], [11], [12], [13], [14]. Furthermore, due to the narrow optical band-gap (∼2–2.2 eV) as well as excellent chemical stability, this material was given much renewed attention in photo-catalysts, photovoltaic facilities and for the degradation of organic pollutants and splitting water for hydrogen production [15], [16], [17], [18], [19], [20], [21], [22], [23], [24].
Beside these fascinating properties, bismuth ferrite has some restriction such as weak ferroelectricity, high leakage current density, poor ferroelectric reliability and inhomogeneous weak magnetization [25], [26], [27], [28]. These obstacles are induced by defects and secondary phases. In order to solve such problems and improve physical properties of BFO, many modification have been investigated, including optimizing preparation parameters [29], doping rare earth [Nd3+, Dy3+, Eu3+] or alkaline earth [Ba2+, Ca2+, Sr2+] metal elements instead of bismuth position [30], [31], [32], [33], [34], as well as transition metal ions [Co3+, Cr3+] substituted on the iron position [35], [36], [37]. Moreover, to shift the absorption edge of BFO to the larger wavelength for photocatalytic and photovoltaic applications, similar improvement have been reported [38], [39], [40]. We also reported in other work that Nd substitution in the BFO structure decreases the optical band-gap and improves photocatalytic activity of BFO catalyst [16], [41], [42].
Yttrium-doped BiFeO3 has attracted interest due to the magnetic, electrical and optical properties of these compounds. The radius of yttrium ion (1.04 Å) is smaller than Bi3+ (1.17 Å) and substitution of bismuth ions by yttrium is expect to induce lattice distortion to enhance physical properties of bismuth ferrite [43], [44], [45]. In last decade, various method including solid-state, sol-gel, co-precipitation and hydrothermal methods have been developed in order to synthesize and study the physical properties of nano-sized Y-doped bismuth ferrite [46], [47], [48], [49], [50]. This research work focused on the structural, optical and ferroelectric and magnetic properties of BYFO particles, and the effect of yttrium on thermal properties, as well as, photocatalytic activity of BYFO particles prepared via mechanical activation was less investigated.
In this study, Bi1−xYxFeO3 (x = 0, 0.05, 0.1, 0.15, 0.2 and 0.25) particles were successfully synthesized through a solid-state method. The effect of yttrium content on the morphology, structural, thermal, ferroelectric and magnetic properties have been investigated in detail. Moreover the photocatalytic activity of all samples was evaluated by decomposing MO under visible light irradiation.
Section snippets
Synthesis of BFO and BYFO particles
Bi1−xYxFeO3 (x = 0, 0.05, 0.1, 0.15, 0.2 and 0.25) nanoparticles were synthesized by the solid-state reaction route. A stoichiometric amount of high purity Bi2O3 (>99%, Sigma Aldrich), Fe2O3 (>99%, Sigma Aldrich) and Y2O3 (>99%, Sigma Aldrich) were mixed in a zirconia vial with a stainless-steel ball to powder ration 20:2, isopropyl alcohol as a milling medium and high energy ball milling at 500 rpm for 30 h (using Amin-Asia planetary high energy ball mill). 3 mol% of excess Bi was added to
Structure of as-prepared crystals
Fig. 1 presents the room temperature X-ray diffraction (XRD) patterns of all as-prepared samples in the range of 20 < 2θ < 65. To confirm the phase structure of the ceramics, the Rietveld refinement of XRD patterns was studied. All major peaks can be indexed by characteristic peaks of BFO perovskite phase (JCPDS card No. 86-1518). Small trace of few weak diffraction peaks related to the impurity (secondary) phases like Bi2Fe4O9 and Bi25FeO40 can be seen in all compositions. When yttrium
Conclusions
In summary, using mechanical activation followed by sintering at 810 °C for 2 h, undoped and yttrium-doped bismuth ferrite was successfully synthesized. XRD results and Rietveld refinement show that the compound crystallizes well in the rhombohedral (for x = 0–0.1) and orthorhombic (x ≥ 0.15) and the crystallite was found in the range of 35–53 nm. DTA curves of BiFeO3 and Bi0.8Y0.2FeO3 reveal that the Curie temperature is decreased by substituting yttrium. P-E and J-E analysis show that the
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