International Nano Letters

, Volume 7, Issue 2, pp 133–140

Morphology and photoluminescence of self-assembled CaWO4:Sm3+ microspheres: effect of pH and surfactant concentration

  • Goutam Singh Ningombam
  • Rajmuhon Singh Nongmaithem
Open Access
Original Article

DOI: 10.1007/s40089-017-0206-2

Cite this article as:
Ningombam, G.S. & Nongmaithem, R.S. Int Nano Lett (2017) 7: 133. doi:10.1007/s40089-017-0206-2


Self-assembled CaWO4:Sm3+ microspheres were prepared via surfactant (sodium dodecyl sulfate) mediated hydrothermal method. The effect of pH and the concentration of surfactant on the morphology and photoluminescence of the synthesized phosphors have been studied. Samples were characterized by X-ray diffractometry (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM) and photoluminescence spectroscopy. The microspheres were found to have an average size of 1–2 µm. They were mesoporous in nature and constituted of nanocrystals of about 10–30 nm dimension. The TEM images revealed the interlinking framework of the nano-sized constituents which consequently lead to the formation of mesoporous microspheres. The lowering of pH causes a slight reduction in the size of microspheres which could have been attributed to loss of OH from the nanoparticle surface and subsequent retardation in the adsorption of growing molecular CaWO4:Sm3+ units. Also, as pH increases, crystallinity decreases. The increase in amount of SDS reduced the crystallinity of the materials, destroyed the monodispersity of microspheres and lowered the luminescence output. It was found that lower pH and higher monodispersity of microspheres are quite favourable for high luminescence output.


CaWO4 microspheres Hydrothermal synthesis Lanthanides Luminescence 


The synthesis and fabrication of nano- or microstructures with uniformly well-defined size and morphology is highly important. The physicochemical properties of nanomaterials depend on their size and shape [1, 2, 3]. The frequency of active centres on the exposed facets and the surface energy of nanostructures could induce many novel nanoscale effects and provides technological potentials. For instance, under UV excitation, ellipsoid β-Ga2O3:Dy exhibits higher emission intensity and quantum yield compared to spindles or microspheres [4]. The luminescence intensity of 1-μm hexagonal NaYF4:Yb,Er is weaker than that of 80-nm cubic spherical samples [5]. The weak intensity of luminescence has been attributed to the presence of non-radiative traps. Spherically fine phosphor microparticles also show high luminescence yield as a result of efficiently high packing densities and low light scattering [6].

Alkaline earth tungstates (AWO4; A = Ca, Sr, Ba) has been extensively studied as luminescent hosts, scintillation detectors, optoelectronics, lasers and catalysis [7, 8, 9, 10]. In photoluminescence, tungstate has been gaining interest due to its physical and chemical stability, low phonon threshold energy, wide band gap semiconducting nature and intrinsic blue emission. The WO4 group can generate blue emission (≈420 nm) on absorption of ultraviolet (UV) radiation mostly in the short wavelength region. This intrinsic blue emission arises from charge transfer transitions between O 2p → W 5d states within the WO4 unit. The blue emission can be harnessed for alteration of luminescent properties by doping with rare earth (RE) ions since most of the RE ions can be absorbed in the blue region.

CaWO4 phosphors are synthesized by several methods such as co-precipitation, solid state reaction, hydro/solvothermal (conventional and microwave), electrospinning, spray pyrolysis, sol–gel route, and pulsed-laser deposition. Of these methods, hydrothermal method is proven to be a promising one for the synthesis of low- and high-order novel architectural designs of nanomaterials through a well-controlled manipulation of appropriate reaction parameters such as temperature, time of hydrothermal ageing, pH of reaction, surfactants or other templates [11, 12, 13]. It has an added advantage of relatively low-temperature growth and size-controlled synthesis. Certain reports have been made on the importance of surfactants and polymers such as sodium dioctyl sulfosuccinate (AOT), polyethylene glycol (PEG), polypeptides in the self-assembly and morphology control of nano- or micro-dimensional materials [14, 15, 16, 17]. Nanotubes and hollow microspheres with high monodispersity can be synthesized using surfactant as soft template via microwave-assisted or conventional hydrothermal method.

In this work, 5 at.% Sm3+-doped CaWO4 (hereafter CaWO4:Sm3+) microspheres were synthesized by conventional hydrothermal method in the presence of sodium dodecyl sulphate (SDS). The effect of variation of pH of the reaction medium and surfactant concentration on the morphology and photoluminescence of the phosphor materials has been studied. The mode of assembly and the size variation of the microspheres have been found to influence the luminescence properties.

Experimental details


All chemicals of analytical grades were used as received without further purification. Calcium nitrate tetrahydrate [Ca(NO3)2·4H2O, Himedia, 99% pure], sodium tungstate dihydrate (Na2WO4·2H2O, Sigma-Aldrich, 99.995% pure), samarium nitrate hexahydrate [Sm(NO3)3·6H2O, Sigma-Aldrich, 99.9% pure], sodium dodecyl sulphate (C12H23SO4Na, Sigma-Aldrich, 98.5% pure) were used for the synthesis. Double-distilled water was used as the solvent and reaction medium.

Synthesis of CaWO4:Sm3+ microspheres

In a typical synthesis, 25 mL of 0.02 M SDS solution was mixed with 25 mL of solution containing 0.19 M Ca(NO3)2·4H2O and 0.01 M Sm(NO3)3·6H2O such that the Ca:Sm atomic ratio is 95:5. The mixture was stirred for homogenous complexation of the metal ions with the SDS molecules. To the complex mixture, 25 mL of 0.2 M Na2WO4·2H2O solution was added with constant stirring for an hour to achieve thorough mixing and complete precipitation. The whole mixture was then transferred to a Teflon-lined autoclave and kept in the pre-heated oven at 150 °C for 3 h. The autoclave was then removed and cooled to room temperature. The products were collected by centrifugation, washed with water and acetone. Finally, the products were dried at 40 °C for further analysis. The pH of the reaction was adjusted by addition of NaOH (1 mol L−1) or HCl (1 mol L−1). For the samples prepared at different SDS concentrations, i.e. 50 and 100 mM, the pH is adjusted to 9. The samples prepared at different pH and 25 mM SDS concentration are labelled as 3H25, 5H25, 7H25, 9H25 and 11H25 corresponding to pH 3, 5.2, 7, 9 and 10.8. The samples prepared at 50 and 100 mM SDS (pH 9) are labelled as 9H50 and 9H100.

Characterization of materials

The crystal structure of the prepared samples was characterized by PANalytical’s X-ray diffractometer (X′-PertPRO) with CuKα (1.5406 Å) radiation with Ni filter. The powdered sample was placed in the sample container and it was mounted at the sample holder. The X-ray tube was operated at 20 mA and 40 kV. The X-ray diffraction (XRD) pattern was recorded in 2θ degree ranging from 10° to 60° at step size of 0.05° s−1. Unit cell parameters were calculated using UnitCell Program ©Tim Holland and Simon Redfern. The average size of the crystallite was calculated by the Scherrer’s formula [17]:
$$ d = \frac{0.94\lambda }{\beta cos\theta } $$
where d is the crystallite size; λ the wavelength of the X-ray beam; β the full width at half maximum of a diffraction peak and θ the diffraction angle.

Scanning electron microscope (SEM FEI Quanta 250) operating at accelerating voltage of 20 kV was used to record the morphology of the synthesized samples and transmission electron microscope (TEM JEOL JEM-2100, Japan available at SAIF, NEHU) operating at 200 kV was used for studying the shape and size of the materials. For SEM, samples were sputter coated and dispersed uniformly on a carbon grid. For TEM, powder samples were dispersed in methanol under ultrasonication for an hour. A drop of the dispersed particles was put over the carbon-coated copper grid and evaporated to dryness at room temperature. It was mounted inside the sample chamber. The photoluminescence spectra were recorded using Perkin Elmer LS55 spectrophotometer.

Results and discussion

XRD study

Figure 1 shows the XRD patterns of CaWO4:Sm3+ crystals obtained at different pH and varied surfactant concentration in the range of 10°–60° in 2θ. Eventually, the CaWO4:Sm3+ crystals have scheelite type tetragonal structure in accordance with the standard diffraction data for bulk CaWO4 (JCPDS No. 77-2233). The results indicate that the CaWO4:Sm3+ samples are crystalline and free from impurity phases. The absence of impurity phases indicates the successful doping of Sm3+ ions in the CaWO4 lattice. Further, the change in pH or the varied surfactant concentration has no adverse effect on the crystal phases. The cell parameters were calculated to be a = b = 5.252 Å, c = 11.371 Å and the unit cell volume, V = 313.68 Å3. The crystallite size calculated using the Scherer’s formula corresponding to the diffraction peak of plane (112) was found to be 15–20 nm. Comparative studies of the intensities of the (112) diffraction peaks with the change of pH and surfactant concentration have been shown in Fig. 2a, b. In Fig. 2a, it was observed that the intensity of the (112) diffraction peak was decreased with the increase in pH of the reaction medium. This indicated that the crystallinity of the samples was lowered with the increase in pH of the medium. In Fig. 2b, it was observed that the sample prepared at an increasing amount of SDS has lower diffraction intensity. Thus, the crystallinity of the samples was lowered with the increasing SDS concentration. Meanwhile, the sample prepared at higher 100 mM SDS concentration showed a slight shift of (112) diffraction peak towards larger 2θ angle.
Fig. 1

XRD patterns of the CaWO4:Sm3+ samples: a 3H25, b 7H25, c 9H25, d 9H50 and e 9H100

Fig. 2

XRD patterns showing the change in crystallinity of CaWO4:Sm3+ with a change pH, b concentration of SDS

SEM and TEM study

The SEM images of the CaWO4:Sm3+ samples prepared at different pH are shown in Fig. 3a–f. All the samples have spherical morphology with size less than or equal to 2 µm. The size of the microspheres seemed to become slightly larger with the increasing pH of the reaction medium. However, the monodispersity of the samples prepared at pH 5 and 7 is quite high compared to other samples. Below pH 4, the CMC is decreased [18]. As a result of which, the number of SDS per micelle is decreased and the number of Ca2+ as counter-ions in the Stern layer attaching to the polar head of SDS will be decreased. When the WO42− ions approach the Ca ions, only fewer units of CaWO4 molecules will be formed and merged to obtain CaWO4:Sm3+ nano-/micro-crystals. Above pH 4, the CMC of SDS does not change at all. This is why the CaWO4 microspheres prepared at pH 3 has smaller size compared to that at pH 5 (absence of HCl and NaOH). At pH 7 and higher, the increasing number of OH ions from NaOH will influence the growth of microspheres. The OH ions will get attached to the surface of the CaWO4:Sm3+. This explains the growth of slightly larger microspheres at high pH. In Fig. 4a–f, the SEM images of the samples prepared at different SDS concentrations with pH being 9 are shown. It is quite obvious that particles tend to grow in size randomly as well as the monodispersity is destroyed with increasing surfactant concentration. Larger particles and aggregates of smaller particles were also formed. The change in shape of the CaWO4:Sm3+ particles have been attributed to the change of micellar structure of SDS at different concentrations arising from the intermicellar interactions. Larger micelles could also be formed due to the stronger hydrophobic interactions. That is why the CaWO4:Sm3+ particles prepared at higher SDS concentrations are larger and aggregated particles are obtained.
Fig. 3

SEM images of CaWO4:Sm3+ samples: a 3H25, b 5H25, c 7H25, d 9H25, e 11H25 and f magnified 5H25

Fig. 4

Low- and high-magnification SEM images of (a, b) 9H25, (c, d) 9H50, (e, f) 9H100

The TEM analysis gives further insight into the morphological construction of the microspheres. Figure 5a–f shows the TEM micrographs of samples prepared at pH 9 and 11 (at 25 mM SDS) and at 100 mM (pH 9). The TEM images have shown that 9H25 and 11H25 do not contain particles of uniform dimensions in the nanometer regime. They rather have intertwined or interconnected framework of nanodimensional particles. However, the particles of 11H25 assume a more reasonable shape and size although they exist in aggregates. Roughly, the particles have size in the range of 15–30 nm. Thus, it is quite obvious that the microspheres so formed are aggregates or self-assembled from nanodimensional units and mesoporous in nature. While the sample 9H100 consists of rather granular nanoparticles with size ranging from 10 to 30 nm. Hence, it can be concluded that higher pH and higher SDS concentration are not favourable for formation of assembled mesoporous microspheres.
Fig. 5

TEM images of CaWO4:Sm3+ samples: (a, b) 9H25, (c, d) 11H25, (e, f) 9H100

Photoluminescence study

A typical photoluminescence excitation spectrum of CaWO4:Sm3+ microspheres is shown in Fig. 6. In WO42− groups, ligand to metal charge transfer (LMCT) occurs by excitation of electrons from the O 2p states to W 5d states to yield the excitation band at 240 nm [19]. The low intense excitation peaks in the region of 300–450 nm corresponds to the f–f transition of Sm3+. The exhibition of the LMCT of WO42− group in the excitation spectrum when monitoring emission at 645 nm (Sm3+ emission) indicates an energy transfer from WO42− groups to the activator ion (Sm3+) [20]. The photoluminescence properties of the self-assembled microspheres were studied under UV excitation at 240 nm as shown in Fig. 7. It is obvious that the activator Sm3+ ions exhibit their characteristic emission in the material as a result of energy transfer from WO42− host to them. The four emission bands at 565, 600, 645 and 707 nm correspond to 4G5/2 → 6H5/2, 6H7/2, 6H9/2 and 6H11/2 transitions in Sm3+ ions [21]. According to Judd–Ofelt theory, the electric dipole transitions occur between energy levels differing in ΔJ by more than one unit (as much as six units in some cases) and the emission centre should not be situated at a centre of inversion [22, 23]. The predominance of the electric dipole transition 4G5/2 → 6H9/2J = 2) (which is not commonly observed in other hosts) is due to removal of inversion centre in SmO8 clusters.
Fig. 6

PL excitation spectra of 9H25 CaWO4:Sm3+ microspheres monitoring emission at 645 nm

In Fig. 7a, the dependence of luminescence intensity with pH of the reaction medium is shown. It is observed that the intensity has an inverse relationship with pH. This can be attributed to the decrease of luminescent quencher –OH and increasing crystallinity as the pH decreases. It is observed from the XRD pattern in Fig. 2 that the crystallinity of the constituent nanodimensional particles increases with decreasing pH of the reaction medium. Hence, the increasing crystallinity could be a reason for luminescence enhancement [24]. During the recombination process in insulators, thinly populated non-stoichiometric defects often occur at the surface of oxide materials as the electrons and holes tend to diffuse through the material towards the surface [25]. In CaWO4 materials prepared by hydrothermal methods, defect-related radiative and non-radiative relaxation channels co-exist in the crystals. The competition between these relaxation channels affect luminescence [26]. If the excited emission centre is in the vicinity of the non-radiative channel (quenching centre), the luminescence efficiency is weakened [5]. Such quenching centres are highly populated in samples of low crystallinity. This further added an explanation to increased emission intensity of the hydrothermally prepared samples with increasing crystallinity.
Fig. 7

PL emission spectra of CaWO4:Sm3+ samples prepared at a 25 mM SDS with varying pH and b pH 9 with varying SDS amount. The samples are excited at 240 nm

In Fig. 7b, the emission spectra of CaWO4:Sm3+ samples prepared at different SDS concentrations are shown. The emission intensity is found to decrease with the increasing amount of SDS in the preparation. Several reasons for this observation could be decrease in crystallinity, organic quenching and non-uniform self-assembly of CaWO4:Sm3+ particles. The crystallinity is decreased with the increasing amount of SDS in the reaction medium. Also, adsorption of organic chain onto the particles assembly could serve as a source of energy sink where it is used up in the vibrational relaxation. Further, the uniform self-assembly with quite high monodispersity apparently lowers the surface to volume ratio and hence the surface energy of the nanocrystals. This could reduce the non-radiative channels in the luminescence [27]. But in this case, monodispersity is destroyed and self-assembly turns out to be non-uniform with increasing SDS concentration. Hence, these factors are accountable for decreasing emission intensities. Altogether, the mode of self-assembly and morphology could induce variation in packing densities and the amount of light scattered as a result of which emission intensities vary with pH and surfactant concentration.


In summary, this work presents the successful synthesis of CaWO4:Sm3+ microspheres via conventional hydrothermal method using SDS as soft template. Highly monodipersed CaWO4:Sm3+ microspheres were obtained at different pH and 25 mM SDS concentration. The pH range of 5–7 is found to be quite favourable for highly monodipersed microsphere formation. However, higher concentration of SDS decreased the monodispersity of microsphere and crystallinity. The microspheres are found to be mesoporous in nature with the constituting nanodimensional units having the size of 10–30 nm as revealed from the micrographs of SEM and TEM. Since the CMC of SDS does not vary much with increase of pH, all samples prepared at different pH have almost the same size. While the samples prepared at different concentration of SDS have change in the shape. This could be attributed to the change of micellar structure of SDS in the solution. The lowering of crystallinity of the samples has also been determined by the mechanism of self-assembly in the micellar structure of SDS. All the samples showed pink-red emission upon excitation at 240 nm. The emission intensities of the CaWO4:Sm3+ microspheres decrease with higher pH and higher SDS concentration. The monodispersity index can be a factor in luminescence yield as observed from the emission intensity of CaWO4:Sm3+ microspheres prepared at different SDS concentration. Beside these, the mode of self-assembly and morphology can be an indispensable factor controlling luminescence output. Hence, this work represents a simple method to design the synthesis of self-assembled microspheres.


Goutam S. N. is grateful to University Grants Commission (UGC, New Delhi) for providing Senior Research Fellowship. The authors acknowledged Physics Department, Manipur University for XRD and SEM facility; SAIF, NEHU, Shillong for TEM facility.

Copyright information

© The Author(s) 2017

Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (, which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Authors and Affiliations

  • Goutam Singh Ningombam
    • 1
  • Rajmuhon Singh Nongmaithem
    • 1
  1. 1.Department of ChemistryManipur UniversityImphal ManipurIndia

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