Comparative analysis of efficient Pb dopant in R and R–S blocks of BaFe12O19 structure synthesized by co-precipitation method
Site occupancy plays an important role in the properties of the materials in general, and in the case of ferrites, this makes a significant effect. Barium ferrite has a wide range of applications ranging from everyday applications to sophisticated communication technologies. Two compositions Ba1−xPbxFe12O19 and BaPbxFe12−xO19 (x = 0.0–1.0) were synthesized by co-precipitation method using similar synthesis conditions. The aim was to understand the different behaviors when Pb replaced Ba in R and R* blocks in the first composition, while in the second composition it replaced iron in RSR*S* blocks. Microstructural and morphological variations in both synthesized compositions because of Pb dopant were responsible for affecting all properties. Higher ionic radius (1.76 Å), lower melting point (950 °C) of lead and gradually increased concentration were responsible for generating stresses and distortions of different magnitudes in both compositions. Magnetic and DC electrical characterizations were investigated by applying similar conditions. Higher phase purity and better morphology are obtained when Ba is replaced by Pb. Strong variation in coercivity due to decrease in anisotropic energy is useful in high-density storage devices. For the other composition, when Fe is replaced by Pb, higher resistivity is obtained. The obtained range of resistivity is useful against eddy current losses in high-frequency devices.
KeywordsBaFe12O19 Lead dopant Coercivity Resistivity Smart applications
Barium hexaferrite and strontium hexaferrite after their discovery from 1950s got the attention of researchers. Their applications vary from common life usage to high-level technology like stealth technology. These ferrites have excellent chemical stability and durable properties which make them reliable for long-life applications. These materials also have applications in microwave devices. Common products of M-type materials are magnetic credit cards, bar codes, door catchers and rotors [1, 2]. Crystalline structure of this material has space group P63/mmc, No. 194 and lattice parameters almost in the ranges of a = b = 5.90 Å and c = 23.30 Å. M-type material has large magnetocrystalline anisotropy, high Curie temperature and high magnetization and coercivity [2, 3]. Its high electrical resistivity and coercivity with sufficiently high residual induction allow the researchers to have its usage as permanent magnets with satisfactory specific magnetic energy. Its high resistivity makes this material to be used as magnet in the presence of high-frequency magnetic fields. Their unit cells contain 38O2− anions, 24Fe3+ cations and 2Ba2+, 2Sr2+ and 2Pb2+ cations. High anisotropy energy constant of such materials like Ba-hexaferrite exceeds almost 100 times that of garnet ferrites. The spin orientation of one site, i.e., 4f1 and 4f2, is down, while that of 2a, 2b and 12k is up, which makes it a unique material for many applications. Currently, its smart applications include magnetic recording media, electric motor and absorption of electromagnetic radiation. Such technology is also known as stealth technology [1, 4]. Researchers have also reported that these properties can be modified by substitution of magnetic and nonmagnetic elements. For this, substitution like Al, Sc and Ga particularly oxide dopants like B2O3, Si2O3 and CaO not only modify the growth and morphology but also induce fascinating properties . These properties are modified due to microstructural variations in lattice parameters, particle growth and their morphology. Replacement and occupancy of divalent and trivalent ions in different crystallographic positions changed not only the strength of valence, interatomic strength and angle but also exchange interactions. Combination of magnetic and electrical properties of M-type ferrites makes their use as spintronics which is a new area or field of microelectronics [6, 7]. Substitution of oxide dopants like PbO and Al2O3 is responsible for modifying magnetic properties.
Based on their structures and chemical compositions, barium-based hexaferrites are classified into six main types . In all of these ferrites, Ba can be replaced by Sr, Pb or other elements . According to Gorter’s model of a system of collinear spin structure , the net magnetic moment per molecule is given by the sum of the magnetic moments of magnetic ions in the molecule. Moreover, the substitution of Fe3+ ions with other trivalent cations such as Al3+, Ga3+, Sc3+ and In3+ is also possible. In this way, we can obtain an extremely large number of compounds with considerably different magnetic properties. This fact makes the hexagonal ferrites attractive for different technical applications and interesting for basic studies on the magnetic interactions in insulators . In the present work, Pb substitution in place of Ba and Fe is responsible for modifying the properties. Iron occupancy status in R and R–S blocks, i.e., K-series, has different impacts in comparison with A-series where Pb replaced Ba ions. For phase purity development, sintering to high temperatures and long duration is required. To save energy and time, researchers use different methodologies like low-melting point dopants and modified synthesis methodology. In presently studied compositions, Pb is used as dopant which has low melting point. Both compositions Ba1−xPbxFe12O19 and BaPbxFe12−xO19 (x = 0.0–1.0) were synthesized through low-temperature co-precipitation method. Their magnetic and DC electrical properties were investigated and are compared here.
2 Experimental procedure
Analytical graded chemicals 99.99% pure were used to synthesize these compositions. These chemicals were BaCO3, Fe(NO3)3·9H2O and PbO in solid form. Calculated and measured quantitates were dissolved in known quantities of HNO3, DI-H2O and HCl, respectively. All solutions were formed and mixed together along with fast magnetic stirring at room temperature. For fertilization, M = 5, alkaline NaOH solution was used. All synthesis parameters and related conditions used were optimized during different experiments.
The optimized used parameters were Fe3+/Ba2+ = 12, pH = 13 and M = 5 for NaOH solution. Washing was done to minimize the impurities. This improved the purity as well as homogeneity. Paste-like material was dried in an oven at 110 ± 2 °C. Water contents were evaporated, and dry crispy material was obtained and transformed into pellets.
2.1 Pellets formation
Pellets were formed by applying suitable hydraulic pressure of 1000 lbs/in2 for 5 min. These pellets were sintered at the same temperature, i.e., 965 ± 5 °C, in a box furnace for 3 h. These pellets were used for different characterizations. For identification, samples of Ba1−xPbxFe12O19 composition were given names as A0, A1, A2, A3, A4 and A5 and for BaPbxFe12−xO19 K0, K1, K2, K3, K4 and K5 for x = 0.0–1.0. These pellets were used for different characterizations.
3 Structural analysis
Because of different crystallographic occupancy positions of different ions within structure, exchange interactions also varied which affected magnetic properties.
3.1 XRD structural parameters
Lattice parameters, volume of unit cell and crystal growth mechanism also have different behaviors as reported . Both compositions confirmed it. So compact and dense structure formed, which modified the magnet properties. It was due to higher density of lead (11.34 g/cm3) than that of barium (3.51 g/cm3) and iron (7.87 g/cm3). The obtained grain size lies almost in 50 nm range. It has made these compositions a useful addition toward magnetic recording media and storage devices applications .
Comparison of both graphs showed nonuniform trends in lattice parameters a and c. It was because of higher mobility and nonuniform diffusion of Pb2+ ions in different lattice sites of structure. Figure 2 explains this mechanism. Mobility of lead ions was one big reason for modified morphological trends and dimensional grains growth, which strongly affected the properties.
4 Magnetic properties
DC magnetization automatic measurement and analysis device—Riken Denshi Model BHH-15—were used for this analysis. This machine was used at room temperature. Factors like dopant mobility, occupancy preference, anisotropic energy and higher density of lead (11.34 g/cm3) than barium (3.51 g/cm3) and iron (7.87 g/cm3) were important for affecting these properties. Five crystallographic sites in hexagonal structure are 2a, 2b, 12k, 4f1 and 4f2 which have contribution in defining magnetic properties [12, 13]. Fe3+ ions have higher positive contribution from 2b sites, while there were weak contribution from 12k sites and much weak contribution from 4f1, 4f2 and 2a sites [15, 16].
Maximum energy product also increased as shown in Fig. 3b. Remanence increased because of the net alignment of grain magnetization due to strong intergrain interactions under the applied field. It caused the maximum energy product to increase . Decrease in coercivity and increase in (BH)max were the important parameters for any hard magnetic material to define the merit of this material.
In S and R structures, 12k and 2b sites are very much sensitive particularly when 12k site lies on the boundary of S–R blocks. So 12k–2b interaction played a decisive role in changing the ongoing trend in the all properties particularly in magnetic properties. Because of these reasons, Br and (BH)max decreased at x = 0.2 and 1.0, while its trend increased from 0.4 to 0.8 [19, 20]. It is totally different from A-series as shown in Fig. 3.
5 DC properties
DC characterizations of both compositions were analyzed as a function of temperature from room temperature to 733 K and 750 K for Ba1−xPbxFe12O19 and BaFe12−xPbxO19, respectively. The obtained data were further analyzed in terms of resistivity (ρ), activation energy (∆E) and mobility (µd). Different mathematical expressions used in this analysis are shown in .
5.1 Resistivity, activation energy and mobility
Useful achievements obtained from both compositions are acceptable range of grain size within ~ 50 nm, smart range of coercivity and maximum energy product and range of resistivity. So they are useful for magnetic media storage devices like credit cards and smart microwave applications.
Ba1−xPbxFe12O19 (A-series) and BaFe12−xPbxO19 (K-series) (for x = 0.0–1.0) were synthesized by co-precipitation method at room temperature by applying the same conditions. Both series were sintered at 965 ± 5 °C for 3 h. 70% and 63% purity levels were obtained. Diamagnetic dopant properties affected growth and purity in both compositions. Seventy percentage purity was an improvement from the already reported one. In A-series, lead, a nonmagnetic element, replaced nonmagnetic barium in R blocks only up to 70% which was better than the already reported one. Grain size, coercivity, maximum energy product and range of resistivity are useful achievements obtained from both compositions. Acceptable range of grain size within ~ 50 nm, smart range of coercivity and maximum energy product are useful for magnetic recording media applications, smart storage devices like camcorder and related microwave applications. These magnetic parameters along with modified resistivity can help to design different electronic components against eddy current losses.
Thanks are due to Higher Education Commission (HEC), Pakistan, for providing financial support to complete this project.
Compliance with ethical standards
Conflict of interest
On behalf of all authors, the corresponding author states that there is no conflict of interest.
- 1.Trukhanov SV, Trukhanov AV, Kostishyn VG, Panina LV, Trukhanov V, Turchenko VA, Tishkevich DI, Trukhanova EL, Yakovenkog OS, Matzuig LY (2017) Investigation into the structural features and microwave absorption of doped barium hexaferrites. J Dalton Trans R Soc Chem 46:9010–9021CrossRefGoogle Scholar
- 3.Turchenko VA, Trukhanov SV, Balagurov AM, Trukhanov SV, Trukhanov AV, Turchenko VA, Kostishyn VG, Panina LV, Kazakevich IS, Balagurov AM (2016) Structure and magnetic properties of BaFe11.9In0.1O19 hexaferrite in a wide temperature range (Me = In3+ and Ga3+(x = 0.1–1.2)). J Alloy Compd 689:383–393CrossRefGoogle Scholar
- 5.Trukhanov SV, Trukhanov AV, Turchenko VA, Trukhanov AV, Tishkevich DI, Trukhanova EL, Zubar TI, Karpinsky DV, Kostishyn VG, Panina LV, Vinnik DA, Gudkova SA, Trofimov EA, Thakur P, Thakur A, Yang Y (2018) Magnetic and dipole moments in indium doped barium hexaferrites. J Magn Magn Mater 457:83–96CrossRefGoogle Scholar
- 11.Albanese G (1977) Recent advances in hexagonal ferrites by the use of nuclear spectroscopic methods. J Phys 4:C1–C85Google Scholar
- 17.Stöhr J, Siegmann HC (2006) Magnetism: from fundamental to nanoscale dynamics, 1st edn. Springer, Berlin, pp 1–234Google Scholar