KnE Materials Science | Sino-Russian ASRTU Conference Alternative Energy: Materials, Technologies, and Devices | pages: 14–23

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1. Introduction

The Bi 2 O 3 -based complex oxides show ion conductive, catalytic, ferroelectric, and magnetic properties [1–3], as well as different structure types, such as fluorite-related structures, pillar or layered Aurivillius phases, or one-dimensional phases [1–4]. The illustration of the last one is column-type compound Bi 26 Mo 10 O 69-d (also named as Bi 13 Mo 5 O 34.5-d ). The Bi 26 Mo 10 O 69 has a unique structure containing [Bi 12 O 14 ] n columns, [MoO m ] polyhedra, and `isolated' Bi ions. Bi 26 Mo 10 O 69 crystallizes in monoclinic symmetry at the temperature above 310 C; below this temperature it exhibits a triclinic distortion. The structure of the monoclinic form was described in [5] with following unit cell parameters: a = 11.74, b = 5.80, c = 24.79 Å, β = 102.84 with P2/c space-group symmetry. The monoclinic model also includes [Bi 12 O 14 ] n columns, `isolated' Bi ions, and MoO 4 tetrahedra; the total quantity of oxygen position being only 68 per one unit cell. The structure of triclinic form with additional oxygen position was suggested in [6]. It includes MoO 5 polyhedra and MoO 5 –MoO 4 chains.

Ordinary substitution in Bi 26 Mo 10 O 69 can be realized by doping molybdenum sublattice or `isolated' bismuth positions resulting to the general formula Bi 26-2x Me 2x Mo 10-2y Me' 2y O 69-d . They exhibit one-dimensional oxygen-ionic conductivity at mediate temperatures and photocatalytic properties [5–7]. Bi 26 Mo 10-2y Me” 2y O 69-δ (Bi 13 Mo 5-y Me” y O 34±δ ) solid solutions were synthesized with 4 or 6 coordinated dopants [5] such as Me”= Li, Mg, Al, Si, Ge [8]; V, P, W [9], etc. The compounds with formulae Bi 26-2x Me' 2x Mo 10 O 69-δ (Bi 13-x Me' x Mo 5 O 34±δ ) were described for 8-coordinated dopants [5], such as Ln [10] or Ca, Sr, and Ba [9]. Double substituted Bi 26 Mo 10 O 69 has been uncommon and was described, for example, for (Ca, Sr) 2 Bi 24 Mo 8 (Cr, W) 2 O 68 [11]. Changes of physicochemical characteristics are both positive and negative results from these substitutions. The present work is devoted to synthesis, investigation, and comparison of Ba-, Mn-, S-, and P- substituted Bi 26 Mo 10 O 69 .

2. Methods

The powders of Bi 26-2x Mn 2x Mo 10 O 69-d , Bi 26-2x Ba 2x Mo 10 O 69-d , Bi 26 Mo 10-2 y S 2 y O 69-d , and Bi 26 Mo 10-2 y P 2 y O 69-d (0.0 x, y 1) solid oxides were synthesized by conventional solid state methods from initial oxides and ammonia salts. Stoichiometric amounts of oxides were weighed, ground in an agate mortar with the ethyl alcohol as a homogenizer, and pelleted using uniaxial press. The pellets were placed in the alumina crucibles on the `powder bed', heated at 823 K for 48 h, and then quenched at air to room temperature. After following regrinding and re-pelletizing, the samples were once more reheated to 1123 K for 24 h and cooled slowly in air to room temperature over a period of approximately 12 h. The concentration ranges of solid solutions and crystal forms of substituted Bi 26 Mo 10 O 69-d were determined by XRPD. X-ray powder diffraction data were obtained on a Bruker Advance D8 diffractometer with a VANTEC1 detector, β-filtered Cu K α radiation, θ / θ geometry, 2 θ range 5–70 , in steps of 0.0211 , with an effective scan time of 1 s per step. For full profile refinement, the data were collected in the 2 θ range 5–133 with an effective scan time of 1649 s per step. DIFFRAC Plus Eva with TOPAS, PDF4 (ICDD) database, and CELREF software was used for the phase analysis. Hydrostatic weighing was used for investigating density of ceramic pellets coated with a moisture-resistant coating. The volume porosity of ceramic samples was obtained by comparison experimental and theoretical (X-ray) density of the samples. The grain size of the powders was estimated by a nanoparticle size analyzer (Shimadzu SALD-7101). The morphology of powders and sintered ceramic samples was carried out using a JEOL JSM 6390LA with EDX-analyzer JED 2300. Photocatalytic properties of Ca 1-3x Bi 2x Ф x MoO 4 series were investigated for degradation of Rhodamine B (RhB) undo UV irradiation. The UV experiments were conducted in a photochemical reactor made of a jacketed quartz tube. A medium-pressure mercury vapor lamp HPL-N (Philips) of 125 W was used as an illuminating source. Temperature of the solution was 40˚C during experiment. The RhB solution concentration were 25 ppm with a catalyst loading of 1 kg/m 3 . Samples were collected at regular intervals for subsequent analysis by spectrophotometer Unico 2800 (552 nm). Impedance measurements were used for conductivity characterization. The samples were pelletized at 20 bar to yield pellets of 10 mm diameter and ca. 3–4 mm thick and sintered at 1123 K during 24 h. Pt electrodes were obtained by covering the end surfaces of pellets by suspension of NH 4 (PtCl 6 ) in ethanol with following drying and decomposition to the Pt. The impedance measurements were carrying out in the range of 523–1123 K on an Elins Z-3000 impedance spectrometer over the respective frequency ranges 3 MHz to 10 Hz. For analysis of impedance plots, the equivalent electrical circuits method was used (Zview software, Version 2.6b, Scribner Associates, Inc.).

3. Results

The forming of Bi 26-2x Me' 2x Mo 10 O 69-d and Bi 26 Mo 10-2 y Me” 2 y O 69-d solid solutions was observed up to x = 0.8 for Me' = Mn, x = 0.7 for Me' = Ba, y = 0.7 for Me' = P, and y = 0.6 for Me' = S. The electron microscopy measurement confirmed these homogeneity ranges. The low concentration of dopant (x,y < 0.1–0.3) leads to triclinic forms of doped Bi 26 Mo 10 O 69-d, high dopant content (x,y > 0.1–0.3) produces the stabilization of monoclinic form of Bi 26 Mo 10 O 69-d –based solid solutions. The unit cell parameters of doped Bi 26 Mo 10 O 69-d show a good correlation with Vegard's law within these ranges (Figure 1). For S-doped samples, the gap caused by changing of coordination is observed at the curves of unit cell parameters.

Figure 1

Unit cell parameters as a function of concentration of dopant in Bi 26-2x Me' 2x Mo 10 O 69-d and Bi 26 Mo 10-2 x Me” 2 x O 69-d compounds.

fig-1.jpg

Refining of structure of Bi 26-2x (Mn, Ba) 2x Mo 10 O 69-d and Bi 26 Mo 10-2 y (S,P) 2 y O 69-d series gives strong information about substitution of isolated Bi positions by Mn or Ba and substitution of Mo positions by S and P. The IR FT spectra of Bi 26 Mo 10-2 y (S,P) 2 y O 69-d samples (Figure 2) show presence of PO 4 and SO 4 groups [12,13]. On the contrary, additional absorption bands for the Bi 26-2x (Mn, Ba) 2x Mo 10 O 69-d series are not observed. The Mo–O at 680–900 cm -1 and Bi-O vibrations at 560–400 cm -1 are indexed by [14–16] and present at IR FT spectra of all the samples.

Figure 2

Typical IR FT spectra of Ba-, S-, and P- substituted Bi 26 Mo 10 O 69 and parent compound.

fig-2.jpg

The grain size of powdered samples was determined by SEM and laser diffraction to be in the range of 1–20 μm. At the following step of research, the samples of substituted Вi 26 Mo 10 O 69-d were pelleted and annealed at 1123 K for 12 hours. As an example, the images of the powder and surface and cross-section of Вi 26 Mo 10 O 69-d –based ceramics are shown in Figure 3. Scanning microscopy showed essential grain growth. Big grains (about dozens of microns) and isolated spherical pores are seen in massive ceramics, indicating the formation of dense. Hydrostatic weighing of the sintered ceramic pellets of the Вi 26 Mo 10 O 69-d –based ceramic revealed a high density of the sintered pellets. The magnitude of an experimental density reaches 97–99% of theoretical (X-ray) density, which corresponds to the 1–3% of porosity of the sintered ceramic pellets.

Figure 3

SEM-images of (a) & (c) ceramic and (b) & (d) powder of (a) Ba, (b) S, (c) Mn, and (d) P substituted Bi 26 Mo 10 O 69 ; (a) & (c) secondary and (b) & (d) backscattering electrons, scale (c) 1:1700, (a), (b), & (d) 1:2000.

fig-3.jpg
Figure 4

Typical impedance spectra of substituted Bi 26 Mo 10 O 69 samples at the high and low temperature ranges.

fig-4.jpg
Table 1

Conductivity values of the selected of Ba-, Mn-, S-, and P- substituted Bi 26 Mo 10 O 69 .


Compound σ 623K , S·cm -1 σ 1023K , S·cm -1
Bi 26 Mo 10 O 69-d 6.45 × 10 -5 6.90 × 10 -3
Bi 25.4 Mn 0.6 Mo 10 O 69-d 4.86 × 10 -6 3.72 × 10 -3
Bi 25.6 Ba 0.4 Mo 10 O 69-d 6.30 × 10 -5 8.31 × 10 -3
Bi 26 Mo 9.8 P 0.2 O 69-d 1.58 × 10 -4 9.37 × 10 -3
Bi 26 Mo 9.6 S 0.4 O 69-d 1.57 × 10 -4 7.77 × 10 -3
YSZ 3 × 10 -5 – 3 × 10 -4 1 × 10 -1 – 3.16 × 10 -2
Figure 5

3D thermal and concentration curves of conductivity of Ba-, Mn-, S-, and P- substituted Bi 26 Mo 10 O 69 .

fig-5.jpg
Figure 6

Typical time dependences of degree of conversion and kinetic curves of RhB for substituted Bi 26 Mo 10 O 69 .

fig-6.jpg

The electro-conductive properties of the ceramic samples of substituted Bi 26 Mo 10 O 69-d were investigated with the impedance spectroscopy. In general, complex plane plots were similar for all compounds. At the relatively high temperatures ( 873–1123 K), an impedance curve consisted of depressed unsymmetrical semi-circle (Figure 4(a)), which could be described by one resistor and two groups of parallel R-CPE connections (R was resistor, CPE was constant phase element). Capacity parameters of both CPE were 10 -5 –10 -4 F; therefore, R-CPE parallel connections corresponded to electrochemical processes at the electrodes [17]. The total resistivity of the sample corresponded to left intercept of spectra in its high frequency part. At relatively low temperatures ( 523–823 K, Figure 4(b)), an impedance spectra consisted of slightly depressed semi-circle in the high frequency part associated to the straight line at the low frequencies. In this case, high frequency part represented the bulk resistivity of the sample [17]; low frequency parts of spectra represented diffusion processes and could be well simulated using Warburg elements or by a pair of parallel R-CPE connections (with capacity parameters 10 -7 –10 -6 F and exponential parameter close to 0.5). As a result, the temperature and dopant concentration curves of conductivity were plotted (Figure 5). Samples with highest conductivity values are shown in Table 1. The conductivity values were comparable with the well-known ionic conductors, for example, YSZ [18].

Control experiments were carried out for RhB oxidation with and without catalyst at visible light (24 hours) and RhB oxidation with catalyst at dark (24 hours). Irreversible absorbance of RhB at catalysis or RhB oxidation undo visible light was not detected. Investigation of the Bi 26 Mo 10 O 69-d -based solid solutions show a small decrease of the photocatalytic activity with dopant concentration. It was suggested that in doped Bi 26 Mo 10 O 69-d a raise of crystal syngony from triclinic to monoclinic led to the slower adsorption and desorption processes. The examples of time dependences of degree of conversion and kinetic curves of RhB are shown in Figure 6. Concentration of RhB changes by Rate law C = C 0· exp(–kt), where C is concentration of RhB, C 0 is initial concentration of RhB, k is reaction rate constant, t is time, as a result pseudo-first order reaction is observed. Results show that reaction rates decrease with dopant concentration by a factor of 1–1.5.

4. Conclusion

In the present research, the possibility of the substitution of Bi 26 Mo 10 O 69 by Ba-, Mn-, S-, and P was shown. Doping of isolated Bi positions by Mn or Ba and substitution of Mo positions by S and P was detected. It was revealed that complex oxides were good ionic conductors and possible photocatalyst.

Funding

This study was supported by RFBR (project №16-33-60026).

References

1 

Vedrine J. C., Coudurier G., Forissier M., Volta J. C., Catalytic properties of metallic oxides in partial oxidation reactions, Materials Chemistry and Physics, Year: 1985, Volume: 13, Issue: 3-4, Page: 365-378. DOI: 10.1016/0254-0584(85)90065-3

2 

Zhao X., Xu T., Yao W., Zhu Y., Synthesis and photoelectrochemical properties of thin bismuth molybdates film with various crystal phases, Thin Solid Films, Year: 2009, Volume: 517, Issue: 20, Page: 5813-5818. DOI: 10.1016/j.tsf.2009.02.135

3 

Boivin J.-C., Structural and electrochemical features of fast oxide ion conductors, International Journal of Inorganic Materials, Year: 2001, Volume: 3, Issue: 8, Page: 1261-1266. DOI: 10.1016/S1466-6049(01)00118-0

4 

Sharma N., Macquart R. B., Christensen M., Avdeev M., Chen Y.-S., Ling C. D., Structure and crystal chemistry of fluorite-related Bi38Mo7O78 from single crystal X-ray diffraction and ab initio calculations, Journal of Solid State Chemistry, Year: 2009, Volume: 182, Issue: 6, Page: 1312-1318. DOI: 10.1016/j.jssc.2009.02.030

5 

Vannier R. N., Mairesse G., Abraham F., Nowogrocki G., Bi26Mo10Oδ solid solution type in the Bi2O3-MoO3-V2O5 ternary diagram, Journal of Solid State Chemistry, Year: 1996, Volume: 122, Issue: 2, Page: 394-406. DOI: 10.1006/jssc.1996.0133

6 

Ling C. D., Miiller W., Johnson M. R., Richard D., Rols S., Madge J., Evans I. R., Local structure, dynamics, and the mechanisms of oxide ionic conduction in Bi26Mo10O69, Chemistry of Materials, Year: 2012, Volume: 24, Issue: 23, Page: 4607-4614. DOI: 10.1021/cm303202r

7 

Muktha B., Aarthi T., Madras G., Guru Row T. N., Substitution effect on the photocatalytic degradation by the series A xBi26-xMo10O68+0.5y (A = Ba, y = 0; A = Bi, La, y = 2): A kinetic study, The Journal of Physical Chemistry B, Year: 2006, Volume: 110, Issue: 21, Page: 10280-10286. DOI: 10.1021/jp060945o

8 

Bastide B., Enjalbert R., Salles P., Galy J., Ionic conductivity of the oxide family Bi[Bi12O14][(Mo,M)O4]5 with M=Li, Mg, Al, Si, Ge and V, Solid State Ionics, Year: 2003, Volume: 158, Issue: 3-4, Page: 351-358. DOI: 10.1016/S0167-2738(02)00910-4

9 

Vannier R.-N., Danzé S., Nowogrocki G., Huvé M., Mairesse G., New class of mono-dimensional bismuth-based oxide anion conductors with a structure based on [Bi12O14]∞ columns, Solid State Ionics, Year: 2000, Volume: 136-137, Page: 51-59. DOI: 10.1016/S0167-2738(00)00351-9

10 

Galy J., Salles P., Rozier P., Castro A., Anionic conductors Ln2/3[Bi12O14](MoO4)5 with Ln = La, Nd, Gd, Ho, Yb. Synthesis-spark plasma sintering-structure-electric properties, Solid State Ionics, Year: 2006, Volume: 177, Issue: 33-34, Page: 2897-2902. DOI: 10.1016/j.ssi.2006.07.059

11 

Muktha B., Guru Row T. N., Crystal structure and ionic conductivity of the series A2Bi 24Mo8X2O68 (A = Ca, Sr and Ba and X = Cr and W) in the Bi2O3-MoO3 system, Structural Chemistry, Year: 2007, Volume: 18, Issue: 2, Page: 195-202. DOI: 10.1007/s11224-006-9093-2

12 

Smith D. H., Seshadri K. S., Infrared spectra of Mg2Ca(SO4)3, MgSO4, hexagonal CaSO4, and orthorhombic CaSO4, Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy, Year: 1999, Volume: 55, Issue: 4, Page: 795-805. DOI: 10.1016/S1386-1425(98)00206-6

13 

He X., Guan M., Lian N., Sun J., Shang T., Synthesis and luminescence characteristics of K2Bi(PO4)(MO4):Eu3+(M = Mo,W) red-emitting phosphor for white LEDs, Journal of Alloys and Compounds, Year: 2010, Volume: 492, Issue: 1-2, Page: 452-455. DOI: 10.1016/j.jallcom.2009.11.138

14 

Li H., Li K., Wang H., Hydrothermal synthesis and photocatalytic properties of bismuth molybdate materials, Materials Chemistry and Physics, Year: 2009, Volume: 116, Issue: 1, Page: 134-142. DOI: 10.1016/j.matchemphys.2009.02.058

15 

Mani M. K., Viola G., Reece M. J., Hall J. P., Evans S. L., Fabrication of carbon nanotube reinforced iron based magnetic alloy composites by spark plasma sintering, Journal of Alloys and Compounds, Year: 2014, Volume: 601, Page: 146-153. DOI: 10.1016/j.jallcom.2014.02.169

16 

Sammes N. M., Tompsett G., Cartner A. M., Characterization of bismuth lead oxide by vibrational spectroscopy, Journal of Materials Science, Year: 1995, Volume: 30, Issue: 17, Page: 4299-4308. DOI: 10.1007/BF00361509

17 

Irvine J. T. S., Sinclair D. C., West A. R., Electroceramics: characterization by impedance spectroscopy, Advanced Materials, Year: 1990, Volume: 2, Issue: 3, Page: 132-138. DOI: 10.1002/adma.19900020304

18 

Joo J. H., Choi G. M., Electrical conductivity of YSZ film grown by pulsed laser deposition, Solid State Ionics, Year: 2006, Volume: 177, Issue: 11-12, Page: 1053-1057. DOI: 10.1016/j.ssi.2006.04.008

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