Enhanced Photoluminescence and Photocatalytic Efficiency of La-Doped Bismuth Molybdate: Its Preparation and Characterization

Herein, a systematic study of the enhanced physicochemical properties of lanthanide doped (La-doped) bismuth molybdate (Bi2MoO6) is performed. For this purpose, Bi2MoO6 and La-doped Bi2MoO6 were prepared by the sol-gel method. BiCl3, Na2MoO4·2H2O, and LaCl3·7H2O were taken as the main precursors while sodium dodecyl sulfate was used as a surfactant. Both Bi2MoO6 and La-doped Bi2MoO6 were calcined at 650 °C for 2 h. These prepared materials were characterized by spectroscopic techniques such as UV–VIS, FT-IR, XRD, photoluminescence, XPS, along with other techniques such as SEM, TEM, TGA, etc. The investigation of luminescence behavior revealed that the La-doped Bi2MoO6 nanocomposite exhibited much greater luminescence compared to the undoped Bi2MoO6. The photocatalytic behavior of the prepared materials was explored by studying the degradation of methylene blue (MB) at room temperature. The degradation of MB with Bi2MoO6 and La-doped bismuth molybdate were observed to be 68% and 75% @ 45 s, respectively, indicating an enhancement of catalytic performance due to the La doping.


Introduction
Light emitting diodes with higher efficiency (>100,000 h) are a potential solution for the growing needs of urban civilization. Among various materials applied for the preparation of LEDs, indium gallium nitride (InGaN), aluminum gallium nitride (AlGaN) have been found to be more efficient as LEDs. Additionally, various other materials have also been applied for this purpose, such as, borates [1], phosphors [2], MOFs [3], different types of mixed metal oxides including CeO 2 , ZnO, ZnAl 2 O 4 [4], Cr-doped ZnGa 2 O 4 [5]. In recent times, scientists have paid more attention towards the preparation and characterization of trivalent lanthanide doped materials due to their applicability as solid-state laser media, fiber amplifiers, infrared to-visible up-converters, field emission displays [6,7] and, therefore, numerous luminescent materials were synthesized with suitable rare earth activators [Ln 3+ ].
Nanomaterials have gained great importance due to remarkable physicochemical properties such as, catalytic, dielectric and luminescence. These properties can be further enhanced by altering the morphology of the nanomaterials. Among the plethora of nanomaterials, a series of Bi-ion based
The Bi 2 MoO 6 was synthesized by the following method. Sodium dodecyl sulfate (0.576 g, 2 mmol) was dispersed into deionized water with constant stirring and temperature was elevated up to 50 • C. At this temperature sodium molybdate (0.483 g, 2 mmol) was added drop wise followed by drop wise addition of bismuth chloride (0.63 g, 2 mmol) to from sol with continuous stirring. The resulting mixture was stirred for further 2 h, while the temperature was raised to 90 • C. After that the solution was filtered and washed with deionized water and ethanol. The obtained precipitate was dried in oven at 60 • C for 3 h. The dried precipitate was ground into powder by mortar and pestle followed by calcination at 650 • C in furnace for 2 h.
La-doped Bi 2 MoO 6 catalyst was synthesized in a similar manner as described above with a slight modification. The sodium dodecyl sulfate (0.576 g, 2 mmol) was dispersed into deionized water at 50 • C, to this solution sodium molybdate (0.483 g, 2 mmol) was added drop-wise followed by the drop-wise addition of lanthanum chloride (0.742 g, 2 mmol) which yielded a white suspension. To this, bismuth chloride (0.63 g, 2 mmol) was added drop-wise and the resulting mixture was heated at 90 • C under continuous stirring for 2 h which resulted in the formation of yellow precipitate. The obtained precipitate was dried in oven at 60 • C for 3 h. The dried precipitate was ground into powder with a mortar and pestle followed by calcination at 650 • C in furnace for 2 h.

Characterization Techniques
The characterizations of synthesized Bi 2 MoO 6 and La-doped Bi 2 MoO 6 were carried out by using different analytical techniques to understand their morphology and other catalytic activities.
The functional groups in Bi 2 MoO 6 and La-doped Bi 2 MoO 6 were determined by Agilent Technologies Cary 630 Fourier transform infrared (FT-IR) spectrometer (Agilent, Santa Clara, USA). Degradation of dye was recorded by T90+ UV-VIS spectrometer (Perkin Elmer lambda 35, Waltham, MA, USA). The photoluminescence (PL) properties of synthetic materials were analyzed by FLS 1000 photoluminescence spectrometer. BET surface area (NOVA 4200e surface area and pore size analyzer (Quantachrome Instruments, FL, USA)). The XRD analysis of the as-prepared nanocatalyst was carried out using a D2 Phaser X-ray diffractometer (Bruker, Bremen, Germany) with Cu Kα radiation (k = 1.5418 A • ). XPS spectra were measured on a PHI 5600 Multi-Technique XPS (Physical Electronics, Lake Drive East, Chanhassen, MN, USA) using monochromatized Al Kα at 1486.6 eV. Peak fitting was performed using Origin software (2019a), USA. TGA was carried out using a TGA/DSC 1 (Mettler Toledo AG, Analytical, Schwerzenbach, Switzerland).

Photocatalytic Activity Measurements
The catalytic activities of prepared Bi 2 MoO 6 and La-doped Bi 2 MoO 6 catalysts were determined by the degradation of methylene blue (MB) as model reaction in the presence of reducing agent NaBH 4 . We designed three reactions for degradation of MB. The time dependent degradation of methylene blue was examined from decrease in the absorbance observed in the UV-VIS spectra, scanned in the range of 400-800 at room temperature. To evaluate the catalytic activity of the prepared material (a) 5 mL solution of methylene blue was mixed with NaBH 4 (0.2 mL, 0.16 M); (b) same solution in the presence of 2 mg of Bi 2 MoO 6 catalyst at room temperature; and (c) the same solution in the presence of 2 mg of La-doped Bi 2 MoO 6 catalyst at room temperature. The blue color of methylene blue disappeared with time which shows the degradation of methylene blue. The reduction efficiency and degradation were determined by the following equation: where C 0 and C t represent the initial and residual concentration of methylene blue in solution with time.
The reduction of methylene blue followed the reaction mechanism in which electrons passes from the reductant BH 4 − to methylene blue which contains double bond. The Bi 2 MoO 6 and La-doped Bi 2 MoO 6 help to decrease the potential difference between donor and acceptor and facilitate the transfer of electron from BH 4 to MB for the hydrogenation of double bond present in methylene blue. Figure 1 shows the SEM micrograms of the prepared Bi 2 MoO 6 and La-doped Bi 2 MoO 6 nanocomposite. The Bi 2 MoO 6 surface morphology appears to be dense rod-like structures, however, the surface morphology of La-doped Bi 2 MoO 6 is found to be globular and hemispherical particles are engaged coarse granular clustering with high porosity. The TEM images of the prepared Bi 2 MoO 6 and La-doped Bi 2 MoO 6 nanocomposite and their particle size distribution graph is given Figure 2. From the TEM images and the particle size distribution graph (Figure 2a,c) of Bi 2 MoO 6, it is evident that the nanoparticles range from 1-8 nm with a mean size of 3.5 nm, while that of La-doped Bi 2 MoO 6 nanocomposites have a size range of 1-7 nm with a mean size of 3 nm (Figure 2b,d), indicating the effect of doping on the particle size of the composite.

BET Analysis
The synthesized Bi2MoO6 and La-doped Bi2MoO6 nanocomposites were subjected to BET analysis to understand the porosity and it was found to be mesoporous in nature. The surface area of the Bi2MoO6 and La-doped Bi2MoO6 nanocomposite was found to be 1.0 m²/g and 3.4 m²/g, respectively. The pore distribution plot revealed that the surface porosity for both the prepared material is different, the Bi2MoO6 possessed a pore volume in the range of 0.3-2.4 × 10 −3 cm 3 /g, while the La-doped Bi2MoO6 nanocomposite was found to possess a pore volume in the range of 0.6-3.8 × 10 −3 cm 3 /g, which is mostly represents granular materials. [22] The pore distribution plot is given in Figure 3.

BET Analysis
The synthesized Bi2MoO6 and La-doped Bi2MoO6 nanocomposites were subjected to BET analysis to understand the porosity and it was found to be mesoporous in nature. The surface area of the Bi2MoO6 and La-doped Bi2MoO6 nanocomposite was found to be 1.0 m²/g and 3.4 m²/g, respectively. The pore distribution plot revealed that the surface porosity for both the prepared material is different, the Bi2MoO6 possessed a pore volume in the range of 0.3-2.4 × 10 −3 cm 3 /g, while the La-doped Bi2MoO6 nanocomposite was found to possess a pore volume in the range of 0.6-3.8 × 10 −3 cm 3 /g, which is mostly represents granular materials. [22] The pore distribution plot is given in Figure 3.

BET Analysis
The synthesized Bi 2 MoO 6 and La-doped Bi 2 MoO 6 nanocomposites were subjected to BET analysis to understand the porosity and it was found to be mesoporous in nature. The surface area of the Bi 2 MoO 6 and La-doped Bi 2 MoO 6 nanocomposite was found to be 1.0 m 2 /g and 3.4 m 2 /g, respectively. The pore distribution plot revealed that the surface porosity for both the prepared material is different, the Bi 2 MoO 6 possessed a pore volume in the range of 0.3-2.4 × 10 −3 cm 3 /g, while the La-doped Bi 2 MoO 6 nanocomposite was found to possess a pore volume in the range of 0.6-3.8 × 10 −3 cm 3 /g, which is mostly represents granular materials [22]. The pore distribution plot is given in Figure 3.

FT-IR Spectral Analysis
FT-IR spectral data provided valuable information about functional groups present in synthesized Bi2MoO6 and La-doped Bi2MoO6 nanocomposites. The FT-IR spectra of Bi2MoO6 and Ladoped Bi2MoO6 were recorded in the range 4000-400 cm −1 . The spectrum of bismuth nanoparticle showed the peaks at 797 cm −1 is due to (Mo = O). The peak observed at 499 cm −1 was assigned to Bi-O bond [23]. The infrared spectrum of La-doped Bi2MoO6 was compared to that of un-doped bismuth molybdate and a shift was observed in the peaks of Mo-O and Bi-O from 797 cm −1 to 794 cm −1 and 499 cm −1 to 493 cm −1 , respectively. This shift can be attributed to the influence of the dual lanthanum in the host matrix of Bi2MoO6 [24]. The IR spectra of Bi2MoO6 and La-doped Bi2MoO6 nanocomposite is given in supplementary file ( Figure S1).

X-Ray Diffraction Spectroscopy
The XRD pattern of the synthesized sample of bismuth molybdate (BW) is given in Figure 4a. It shows pronounced diffraction peaks of (131), (212), (260), (191) and (280) planes at 2-Theta = 28.271, 47.094, 47.214, 56.283, and 56.452, which can be ascribed to the characteristic orthorhombic phase of Bi2MoO6 (JCPDS card no. 77-1246). However, the lanthanum doped bismuth molybdate (LW) exhibits more than one crystal phases as shown in Figure 4b. It shows the main diffraction peaks of α-Bi2Mo3O12 at 2θ = 27.947°, 29.170°, 30.995°, and 48.348° corresponding to diffraction planes of (221), (023), (040) and (242), respectively, and match with JCPDS card no. 21-0103. It was found that the addition of La to the Bi2MoO6 induced a phase transition of synthesized bismuth molybdenum from γ-Bi2MoO6 to α-Bi2Mo3O12. The diffraction peaks of planes (110), (130), and (213) at diffraction angles 13.55, 30.98 and 37.57, respectively shows the presence of monoclinic crystal phase of lanthanum molybdenum oxide (LaMo5O8). Along with these two phases, the XRD pattern also shows the presence of bismuth oxide (Bi2O3) as presented by the diffraction peaks at 27.94, 46.20, and 54.24 correspond to (201), (222), and (203) planes. Moreover, the crystallite size of the Bi2MoO6 and Ladoped Bi2MoO6 was calculated using Debye-Scherrer equation and the crystallite size obtained was found to be 18 and 14 nm. Normally the size of crystallites as obtained by XRD are smaller than the particle size obtained by TEM, as the particles are made up of crystallites. However, in our case the observation is opposite, this may be because XRD measurements are usually on bulk of the sample, whereas TEM is usually on a small selected area, which in our case showed smaller particle size.

FT-IR Spectral Analysis
FT-IR spectral data provided valuable information about functional groups present in synthesized Bi 2 MoO 6 and La-doped Bi 2 MoO 6 nanocomposites. The FT-IR spectra of Bi 2 MoO 6 and La-doped Bi 2 MoO 6 were recorded in the range 4000-400 cm −1 . The spectrum of bismuth nanoparticle showed the peaks at 797 cm −1 is due to (Mo = O). The peak observed at 499 cm −1 was assigned to Bi-O bond [23]. The infrared spectrum of La-doped Bi 2 MoO 6 was compared to that of un-doped bismuth molybdate and a shift was observed in the peaks of Mo-O and Bi-O from 797 cm −1 to 794 cm −1 and 499 cm −1 to 493 cm −1 , respectively. This shift can be attributed to the influence of the dual lanthanum in the host matrix of Bi 2 MoO 6 [24]. The IR spectra of Bi 2 MoO 6 and La-doped Bi 2 MoO 6 nanocomposite is given in Supplementary File ( Figure S1).

X-Ray Diffraction Spectroscopy
The XRD pattern of the synthesized sample of bismuth molybdate (BW) is given in Figure 4a was calculated using Debye-Scherrer equation and the crystallite size obtained was found to be 18 and 14 nm. Normally the size of crystallites as obtained by XRD are smaller than the particle size obtained by TEM, as the particles are made up of crystallites. However, in our case the observation is opposite, this may be because XRD measurements are usually on bulk of the sample, whereas TEM is usually on a small selected area, which in our case showed smaller particle size.

Luminescence
The optical property of Bi 3+ ions have been explained in terms of Russell-Saunders type electronic energy terms with s 2 configuration in the ground and sp configuration (first excited state). Among these, the energetically lowest possible 3 P0-1 S0 excitation is strongly forbidden but the 3 P1-1 S0 transition is possible because of spin-orbit coupling of the 3 P1 and 1 P1 states [25]. Figure 5 represented the PL spectra of un-doped Bi2MoO6 and La-Bi2MoO6 in the range 350 to 750 nm excited by 350 nm [26]. The relatively broad PL peaks appeared around 700 nm with enhanced emission intensity in Ladoped Bi2MoO6 compared to un-doped Bi2MoO6. PL intensity normally depends on crystallinity, materials having more crystallinity exhibits enhanced PL intensity. [27]. The same possible reason might be attributed to the enhanced emission intensity of La-Bi2MoO6. A similar observation has been reported for CaMoO4:Eu 3+ in the literature [27].

X-Ray Photoelectron Spectroscopy
Surface composition analyses of the prepared nanocomposites were analyzed using X-Ray photoelectron spectroscopy (XPS). The survey scan revealed the presence of Bi, Mo, O elements in the composites prepared, and an additional signal corresponding to the element La revealed the successful doping of La in the nanocomposite given in Figure 6.

Luminescence
The optical property of Bi 3+ ions have been explained in terms of Russell-Saunders type electronic energy terms with s 2 configuration in the ground and sp configuration (first excited state). Among these, the energetically lowest possible 3 P 0 -1 S 0 excitation is strongly forbidden but the 3 P 1 -1 S 0 transition is possible because of spin-orbit coupling of the 3 P 1 and 1 P 1 states [25]. Figure 5 represented the PL spectra of un-doped Bi2MoO6 and La-Bi 2 MoO 6 in the range 350 to 750 nm excited by 350 nm [26]. The relatively broad PL peaks appeared around 700 nm with enhanced emission intensity in La-doped Bi 2 MoO 6 compared to un-doped Bi 2 MoO 6 . PL intensity normally depends on crystallinity, materials having more crystallinity exhibits enhanced PL intensity. [27]. The same possible reason might be attributed to the enhanced emission intensity of La-Bi 2 MoO 6 . A similar observation has been reported for CaMoO 4 :Eu 3+ in the literature [27].

Luminescence
The optical property of Bi 3+ ions have been explained in terms of Russell-Saunders type electronic energy terms with s 2 configuration in the ground and sp configuration (first excited state). Among these, the energetically lowest possible 3 P0-1 S0 excitation is strongly forbidden but the 3 P1-1 S0 transition is possible because of spin-orbit coupling of the 3 P1 and 1 P1 states [25]. Figure 5 represented the PL spectra of un-doped Bi2MoO6 and La-Bi2MoO6 in the range 350 to 750 nm excited by 350 nm [26]. The relatively broad PL peaks appeared around 700 nm with enhanced emission intensity in Ladoped Bi2MoO6 compared to un-doped Bi2MoO6. PL intensity normally depends on crystallinity, materials having more crystallinity exhibits enhanced PL intensity. [27]. The same possible reason might be attributed to the enhanced emission intensity of La-Bi2MoO6. A similar observation has been reported for CaMoO4:Eu 3+ in the literature [27].

X-Ray Photoelectron Spectroscopy
Surface composition analyses of the prepared nanocomposites were analyzed using X-Ray photoelectron spectroscopy (XPS). The survey scan revealed the presence of Bi, Mo, O elements in the composites prepared, and an additional signal corresponding to the element La revealed the successful doping of La in the nanocomposite given in Figure 6.

X-Ray Photoelectron Spectroscopy
Surface composition analyses of the prepared nanocomposites were analyzed using X-Ray photoelectron spectroscopy (XPS). The survey scan revealed the presence of Bi, Mo, O elements in the composites prepared, and an additional signal corresponding to the element La revealed the successful doping of La in the nanocomposite given in Figure 6. The deconvolution of the Bi 4f spectrum of Bi2MoO6 yielded peaks at 161.8 eV and 163.8 eV corresponding to Bi 4f5/2 and the difference in BE between the two Bi 4f5/2 peaks was 2.0 eV, which coincided with that between Bi 0 and Bi 3 . While in the case of La-doped Bi2MoO6 nanocomposite the Bi 4f spectrum yielded peaks at 159.3 eV and 164.6 eV corresponding to Bi 4f7/2 and Bi 4f5/2, respectively. However, the Mo 3d deconvoluted spectrum for the Bi2MoO6 yielded peaks at 234.6 eV and 236.7 eV attributed to Mo 3d5/2 which correspond to the Mo 6+ , while that of La-doped Bi2MoO6 nanocomposite yielded peaks at 233.2 eV, 236.7 eV, and 238.3 eV [28]. The deconvolution of the Bi 4f and Mo 3d spectrum of Bi2MoO6 and La-doped Bi2MoO6 nanocomposites are given in Figure 7.  The deconvolution of the Bi 4f spectrum of Bi2MoO6 yielded peaks at 161.8 eV and 163.8 eV corresponding to Bi 4f5/2 and the difference in BE between the two Bi 4f5/2 peaks was 2.0 eV, which coincided with that between Bi 0 and Bi 3 . While in the case of La-doped Bi2MoO6 nanocomposite the Bi 4f spectrum yielded peaks at 159.3 eV and 164.6 eV corresponding to Bi 4f7/2 and Bi 4f5/2, respectively. However, the Mo 3d deconvoluted spectrum for the Bi2MoO6 yielded peaks at 234.6 eV and 236.7 eV attributed to Mo 3d5/2 which correspond to the Mo 6+ , while that of La-doped Bi2MoO6 nanocomposite yielded peaks at 233.2 eV, 236.7 eV, and 238.3 eV [28]. The deconvolution of the Bi 4f and Mo 3d spectrum of Bi2MoO6 and La-doped Bi2MoO6 nanocomposites are given in Figure 7.

TGA Analysis
Thermogravimetric analysis (TGA) was conducted to identify the thermal behavior of the Bi 2 MoO 6 and La-doped Bi 2 MoO 6 nanocomposites and the results were compared as displayed in Figure 8. TGA of Bi 2 MoO 6 reveals that there is an 8% weight loss when the sample is heated to 800 • C starting from 25 • C at a heating rate of 10 • C/minute under an inert atmosphere. However, when the La-doped Bi 2 MoO 6 was subjected to similar study it is found that the weight loss is up to 16% indicating that the later nanocomposite is thermally less stable than un-doped Bi 2 MoO 6 .

TGA Analysis
Thermogravimetric analysis (TGA) was conducted to identify the thermal behavior of the Bi2MoO6 and La-doped Bi2MoO6 nanocomposites and the results were compared as displayed in Figure 8. TGA of Bi2MoO6 reveals that there is an 8% weight loss when the sample is heated to 800 °C starting from 25 °C at a heating rate of 10 °C/minute under an inert atmosphere. However, when the La-doped Bi2MoO6 was subjected to similar study it is found that the weight loss is up to 16% indicating that the later nanocomposite is thermally less stable than un-doped Bi2MoO6.

Photocatalytic Activity
The catalytic activities of undoped Bi2MoO6 and La-doped Bi2MoO6 were evaluated by the degradation of methylene blue (MB) using UV-visible spectroscopy. λ-max for pure methylene blue was noted at 665 nm. The gradual change in color was observed at different time intervals which ensured the enhanced reduction. Maximum degradation was observed at a time interval of 45 s with complete decolorization. The presence of the reaction intermediates was eradicated as no new band appeared in the spectrum. The degradation of methylene blue using NaBH4 was recorded minimal 18% at 45 s, while in the presence of undoped BiMoO6 catalyst, the degradation of MB was enhanced up to 48% within first 15 s, as the reaction proceeds, the % age degradation was recorded as 55% and 68% at 30 and 45 s, respectively ( Figure 9). However, when a similar reaction was carried out using NaBH4 in the presence of La-doped Bi2MoO6, a drastic increase in the degradation of methylene blue was observed, with a percentage of degradation of 53% in the first 15 s, which further proceeds to 69% and 75% at 30 and 45 s, respectively. The degradation kinetics of the reaction are illustrated graphically in Figure 10.

Photocatalytic Activity
The catalytic activities of undoped Bi 2 MoO 6 and La-doped Bi 2 MoO 6 were evaluated by the degradation of methylene blue (MB) using UV-visible spectroscopy. λ-max for pure methylene blue was noted at 665 nm. The gradual change in color was observed at different time intervals which ensured the enhanced reduction. Maximum degradation was observed at a time interval of 45 s with complete decolorization. The presence of the reaction intermediates was eradicated as no new band appeared in the spectrum. The degradation of methylene blue using NaBH 4 was recorded minimal 18% at 45 s, while in the presence of undoped BiMoO 6 catalyst, the degradation of MB was enhanced up to 48% within first 15 s, as the reaction proceeds, the % age degradation was recorded as 55% and 68% at 30 and 45 s, respectively ( Figure 9). However, when a similar reaction was carried out using NaBH 4 in the presence of La-doped Bi 2 MoO 6 , a drastic increase in the degradation of methylene blue was observed, with a percentage of degradation of 53% in the first 15 s, which further proceeds to 69% and 75% at 30 and 45 s, respectively. The degradation kinetics of the reaction are illustrated graphically in Figure 10.  Relevant literature reveals that similar pattern of degradation has been observed with Pd-Nano-diamond-GO composite for the degradation of MB from 15 s to 60 s [23]. This enhancement of degradation efficiency can be attributed to the inclusion of La in the system. By correlating the characterization data obtained and the results of photocatalytic activity it can be concluded that the inclusion of La leads to the formation of nanocomposites with smaller dimension and larger surface area. These changes along with the phase transformation of γ-Bi 2 MoO 6 to α-Bi 2 Mo 3 O 12, and the presence of monoclinic crystal phase of lanthanum molybdenum oxide (LaMo 5 O 8 ) are assumed to be responsible in the enhancement of photocatalytic activity towards the degradation of MB.
Relevant literature reveals that similar pattern of degradation has been observed with Pd-Nanodiamond-GO composite for the degradation of MB from 15 s to 60 s [23]. This enhancement of degradation efficiency can be attributed to the inclusion of La in the system. By correlating the characterization data obtained and the results of photocatalytic activity it can be concluded that the inclusion of La leads to the formation of nanocomposites with smaller dimension and larger surface area. These changes along with the phase transformation of γ-Bi2MoO6 to α-Bi2Mo3O12, and the presence of monoclinic crystal phase of lanthanum molybdenum oxide (LaMo5O8) are assumed to be responsible in the enhancement of photocatalytic activity towards the degradation of MB. Figure 10. Graphical illustration of the photocatalytic degradation kinetics of methylene blue using NaBH4, NaBH4 in the presence of Bi2MoO6, and NaBH4 in the presence of La-doped Bi2MoO6.

Conclusion
In conclusion the Bi2MoO6 and La-doped Bi2MoO6 materials were successfully synthesized through the environmental friendly sol-gel method using sodium dodecyl sulfate as a surfactant. The morphological and structural properties of the synthesized material were determined by various analytical techniques. The morphology of Bi2MoO6 was changed with lanthanum doping, i.e., from dense rod-like structures to globular and hemispherical particles engaged into clusters with high porosity. The photo-degradation efficiency of La-Bi2MoO6 for MB was enhanced due to lanthanum doping and can be attributed to the efficient separation and preventing of the recombination of electron-hole pairs. Hence, the environmentally friendly sol-gel method for synthesis of La-Bi2MoO6 is an efficient tool for possible applications in the degradation of dyes and sequestering of MB pollutants from environment, and this study can be further extended to other pollutants, which is in progress and shall be published later.

Conclusion
In conclusion the Bi 2 MoO 6 and La-doped Bi 2 MoO 6 materials were successfully synthesized through the environmental friendly sol-gel method using sodium dodecyl sulfate as a surfactant. The morphological and structural properties of the synthesized material were determined by various analytical techniques. The morphology of Bi 2 MoO 6 was changed with lanthanum doping, i.e., from dense rod-like structures to globular and hemispherical particles engaged into clusters with high porosity. The photo-degradation efficiency of La-Bi 2 MoO 6 for MB was enhanced due to lanthanum doping and can be attributed to the efficient separation and preventing of the recombination of electron-hole pairs. Hence, the environmentally friendly sol-gel method for synthesis of La-Bi 2 MoO 6 is an efficient tool for possible applications in the degradation of dyes and sequestering of MB pollutants from environment, and this study can be further extended to other pollutants, which is in progress and shall be published later.