Journal of Minerals and Materials Characterization and Engineering
Vol.06 No.03(2018), Article ID:84898,10 pages

Structural Role of Cerium Oxide in Lead Silicate Glasses and Glass Ceramics

Gomaa El-Damrawi1*, Amal Behairy2

1Physics Department, Faculty of Science, Mansoura University, Mansoura, Egypt

2The High Institute of Engineering and Technology, New Damietta, Damietta, Egypt

Copyright © 2018 by authors and Scientific Research Publishing Inc.

This work is licensed under the Creative Commons Attribution-NonCommercial International License (CC BY-NC 4.0).

Received: April 16, 2018; Accepted: May 27, 2018; Published: May 30, 2018


Silicate glasses and glass ceramics in the system CeO2-PbO-SiO2 have been studied as a function of the structure factors R and K. The latter two factors are defined as: R = (CeO2 + PbO)/SiO2 and K = (SiO2/CeO2) molar ratios. In this glass, PbO is fixed at 50 mol% and CeO2 increases at the expense of SiO2. NMR investigations have revealed that increasing R which is accompanied with decreasing K leads to reasonable decrease in the shielding of silicon atoms. The chemical shift (δ) showed an increasing behavior due to increasing non-bridging oxygen atoms (NBO) in silicate network. It is evidenced that NBO in cerium free glass is much lower than that of glasses containing CeO2. Increasing R is clearly leading to higher chemical shift and higher NBO. This reflects that CeO2 has an effective structural role, since it would be consumed in all cases as an intermediate oxide. The main portions from CeO2 and PbO inter as glass modifiers which are consumed to form NBO atoms. A limited portion of CeO2 acts as glass former which consumed to form tetrahedral cerium containing NBO due to modification by PbO as a modifier oxide. Increasing R = [(CeO2 + PbO)/SiO2] from 1 to 2.34 leads to a frequent increase of NBO in the average glass network. FTIR spectroscopy of the glasses showed a clear shift of the main absorbance peak toward the low wavenumber with increasing R which confirms the increasing silicate units containing NBO atoms. XRD of the investigated materials revealed the presence of some nanostructures from cerium silicate crystalline phases. Formation of separated phases containing micro clusters is found to depend on NBO concentration, since NBO can facilitate process of phase separation. Majority of modifier are consumed to form NBO in the glass network and the rest are aggregated or separated to form silicate phase riches with cerium cations. In such case, some of silicon atoms are electrically compensated with both Pb and Ce cations.


Cerium in Glasses, Crystalline Clusters, NMR Feature, Glass Ceramics

1. Introduction

Glass ceramics containing PbO are useful to be studied because of their importance in several fields of applications [1] [2] [3] [4] [5] . PbO can easily resist devitrification process and enhances durability of the glasses. Recently, the continuous progress of the materials containing cerium and lead oxide has been requiring immediate attention in viewpoint of both academic [6] [7] and bio-applications [8] [9] [10] [11] . Structural role of PbO and CeO2 as network intermediates is documented in several types of glasses [3] [4] [5] . This dual role is depending on their content, glass composition and the type of glass. PbO can modify silicate network similar to alkali oxide particularly at low concentration [12] [13] . In such situation, the modifiers are consumed to form silicate units containing NBO atoms [12] [13] [14] . In glasses enriched with lead, PbO4 species would be formed and directly affects the glass structure through forming Pb-O-Si bonds [5] [13] .

Structure of cerium borate and borosilicate glasses has been recently investigated via FTIR and NMR spectroscopy [6] [7] [15] [16] [17] . The obtained results have proved that cerium ions have a role of a network intermediate. Although several investigations have been done to characterize micro-structure of lead silicate glasses, the role of PbO and CeO2 in studied silicate glass ceramics has not been fully explored. Our aim, in this study is to offer more information on the short range structure of cerium lead silicate glass ceramics in a wide range of composition. In particular, we focus on the short range ordered structure around the Si atoms via 29Si NMR techniques. In addition, the role of cerium ions as an agent for phase separation and crystallization has also to be studied. In this regard, glasses are investigated with SEM , FTIR, XRD spectroscopies and the obtained data is compared with that of base glass, free from CeO2.

2. Experimental

Glass samples containing different concentrations from CeO2, PbO and SiO2 have been prepared by mixing the desired components in silica crucibles. The crucible and its content was transferred into an electric furnace and the temperature is raised gradually to reach the limit suitable for melting. The melting temperature is ranged between 1350˚C -1450˚C, depending on the material composition. The melt was swirled severally to ensure homogeneity and to get bubble free matrix. Finally, the melt was poured between two stainless steel plates. The obtained samples are transferred to another furnace and annealed at 350˚C to reduce internal stress. The samples are obtained in disc like shape of 2 mm thickness and 5 mm radius.

2.1. 29Si NMR Measurements

Fine powdered samples of different compositions have been investigated by using JEOL GSX-500 high-resolution solid state MAS NMR spectrometer of magnetic field of 11.74 T (Mansoura University-EGYPT). Spectra of silicon nuclei were recorded at a frequency of 99.3 MHz. A spinning rate of 7 kHz has been applied by using zirconia sample holder. An electric Pulse of 2.62 μs length and of 30 s recycle delay are used. Several scans (10,000 - 12,000) were acquired to get high resolution NMR spectra.

2.2. X-Ray Diffraction Method

XRD measurements were undertaken using a Bruker D5005 diffractmeter, at 40 kV - 30 mA power. Scans were taken between 10˚ - 70˚ with 0.04˚ increments, 15 - 30 seconds/increment.

2.3. Infrared Spectra (IR)

The FTIR absorption spectra were obtained, by KBr pellets technique, at room temperature in the range 400 - 4000 cm−1 using Mattson 5000 FTIR spectrometer with a spectral resolution of 2 cm−1. The glass powder of 0.02 g was mixed with a 0.2 g of KBr and pressed to form a thin disc. At least three samples of each glass were analyzed. The spectrum of each sample is obtained due to collected 20 scans. The obtained spectrum was normalized to the spectrum of blank KBr pellet; i.e. a pure KBr spectrum was subtracted from each glass spectrum. In addition, the spectra were corrected to the background and dark currents using two-point baseline correction. Then the spectra were normalized by making the absorption of each spectrum varies between 0 and 1 arbitrary unit. In addition such normalization is necessary to eliminate the concentration effect of the powder sample in the KBr disc.

3. Results and Discussion

NMR spectra of glasses having different R values (1, 1.2. 1.86 and 2.34) are shown in Figures 1(a)-(d). As shown from this figure, there is a remarkable shift in center of the main peak position of 29Si NMR spectra with increasing R, i.e. increasing CeO2 concentrations. The NMR resonance peak centered at −87.3 ppm in cerium free glass (spectrum a) is shifted clearly toward much higher value (−75.4 ppm) in glass of 20 mol% CeO2 (R = 2.34). Increasing chemical shift of the silicate nuclei with increasing (PbO + CeO2) concentration is attributed to the modification role of both cerium and lead oxides. In addition, decreasing of SiO2 concentration as a result of increasing CeO2 and decreasing K will result in increasing NBO per SiO2 groups.

In terms of Qn notation, (Q is silicon atom and n is the number of bridging bonds between Si and oxygen atoms), chemical shift value of base glass (−87.3 ppm) is attributed to mixture of Q3 and Q2 (silicate unit containing three and two bridging oxygen atoms as a major portion). In addition, little of Q2[OPb] configurations may also be present [18] [19] . The main NMR resonances centered at −83.3, −77.8, and −75.4 ppm in glasses of R = 1.2, 1.68 and 2.34 (CeO2 = 5, 15 and 20 mol% CeO2) show that silicate network is frequently deshielded by the effect of increasing the modifier oxide concentration. In glass of R = 1.2 and

Figure 1. NMR spectra of silicon nuclei of cerium free, R = 1 (a) and of glasses containing 5 and 15 and 20 mol% CeO2, R = 1.2, 1.86 and 2.34 ((b)-(d), respectively).

containing 5 mol% CeO2, Q2 species are the dominant. On the other hand, glasses containing 15 and 20 mol% CeO2 (R = 1.68 and 2.34) contain Q1 and Q0 species respectively. In addition few silicate units containing cerium oxide in the second coordination sphere are suggested to be present.

The concentration of different silicate units (Qn, n = 0 - 4) could be quantitavely obtained by an integration process which is applied to all NMR spectra of silicon nuclei. Figure 2 is presented as an example for the deconvolution process. From spectral analysis, the corresponding percentage of Q1 = 17%, Q2 = 55%, Q3 = 20%, and Q4 = 8% characterize binary lead silicate glass are simply evidenced. On the other hand, the values of Q0 = 29%, Q1 = 44%, Q2 = 23%, Q3 = 4% and Q4 = 0% are obtained values characterize ternary cerium lead silicate glass of R = 1.86. This leads one to confirm that the major portion from CeO2 and PbO can be introduced as glass modifier, since silicate units contain a mixture from Q1 and Q0 types are formed with higher concentration than that of Q2 and Q3 in glass free from CeO2. In such glass, some of Qn would contain Ce or Pb or both in the second coordination sphere of silicon. As a result, Si-O-Ce and Ce-O-Pb configurations are formed. These linkages are known to deshield the silicon nuclei in comparison with Si-O-Si linkages.

Figure 3 presents the change of the average isotropic chemical shift (δ) of 29Si nuclei upon increasing R. It can be shown from this figure that δ increases (from −87.3 to −75.4 ppm) with increasing R values i.e. CeO2 contents. This change leads to increasing NBO. Beside, some Si-O-Ce or Si-O-Pb are formed at expense

Figure 2. Separation of NMR spectrum of 50PbO-50SiO2 glass into different component bands.

Figure 3. Relation between chemical shift of silicon nuclei and (PbO + CeO2)/SiO2 molar ratio.

of the more stronger Si-O-Si bonds. This assures that cerium oxide inters the glass as an strong glass modifier. In addition, silicate units of the type Ce[2OSi] containing NBO atoms are formed. As a result NBO, Si-O-Ce and Pb-O-Si bonds can deshield silicate units relative to stronger Si-O-Si bond in glasses of higher modification levels. Increasing deshielding upon increasing CeO2 concentration is the main reason of increasing chemical shift with increasing CeO2 concentration as represented in Figure 3.

To determine the structural role of CeO2 as an effective modifier, it is useful to compare FTIR spectra of cerium containing glasses with that of free CeO2. As an example, Figure 4 shows FTIR spectra of cerium free glass and for glass samples

Figure 4. FTIR spectra of cerium free glass (R = 1) and of that containing 5 (R = 1.2) and 15 (R = 1.86) and 20 (R = 2.34) mol%.

contains 5, 15 and 20 mol% CeO2 as an example. The main band at ca. 960 cm−1 in glass free from cerium oxide is shifted progressively towards 860 cm−1, since the activity of Q2 and Q1 species containing Ce linkages are present in glass containing 5 and 15 mol%. In addition, week envelope represents Q0 is appeared at about 770 cm−1 in the spectra of glass containing 20 mol%CeO2. These changes are clearly evidenced in glass of higher CeO2 oxide (15 and 20 mol% CeO2), see Figure 4. As is shown from this figure, band characterizes Q0 (at 770 cm−1) [20] [21] [22] [23] is simply resolved which confirms that loos silicate units would be formed in high CeO2 to SiO2 molar ratio.

The nature of XRD pattern is known to depend upon the content of NBO in the main glass forming units such as [QnSiO4] and [Qn(PO)3] species [7] [8] [9] . In this regard, the relative ratio of modifier to former is high enough to yield pyrosilicate (Q1, 3NBO) and orthosilicate (Q0, 4NBO) units which have been documented from NMR results. The nonbridging oxygen should be electrically balanced by positive ions (Ce2+). Accumulation of Ce2+ cations around NBO in silicate network will result in producing crystalline clusters of cerium orthosilicate type [7] [8] [9] . These considerations are supported from comparison between XRD pattern of vitreous CeO2 and of that of cerium silicate glass. Both spectra offer sharp diffraction lines at the same position. The intensity of the diffraction pattern of cerium silicate glass is appeared to be lower than that of the pure CeO2. This may because the clusters formed from Ce and O ions are distributed within amorphous silicate units which play the role of lowering the total crystallite species. This argument is further supported, since the sharp diffraction peak is superimposed on a broad hump (between 20˚ - 40˚) which is a characteristic feature of the main amorphous glass network. This observation is simply strengthened from XRD spectra of cerium free glass, Figure 5, since amorphous distribution of glass constituents is the dominant.

Glass contains SiO2 and PbO doesn’t greatly affect the process of crystallization or clustring, but the main changes were found to depend on CeO2. Figure 6 showed that there is a great difference between morphology of glass containing

Figure 5. XRD patterns of glass free from CeO2 (below) and that of glass containing 20 mol% CeO2 together with vitreous CeO2.


Figure 6. SEM of glass containing 20 mol% CeO2 (a) and of glass free from CeO2 (b).

20 mol% CeO2, Figure 6(a) and of cerium free glass, Figure 6(b), since crystalline clusters from cerium silicate phases are clearly resolved in the morphology of sample containing 20 mol% CeO2.

4. Conclusion

NMR investigation has revealed that increasing of CeO2 at the expense of SiO2 at a constant concentration of PbO increases chemical shift (δ) of 29Si nuclei through increasing (NBO) in silicate network. NBO atoms in cerium free glass are much lower than those of glasses containing CeO2. Higher concentration of CeO2 leads to higher chemical shift and higher NBO. The structural role of CeO2 is definitely determined as a modifier oxide in the investigated lead silicate network. FTIR analysis revealed that increasing CeO2 will result in increasing silicate units which are enriched with NBO atoms The major modifiers are consumed to form NBO in silicate network and the few are aggregated to form crystalline silicate phase riches with cerium oxide. XRD patterns of cerium containing glasses reflect the crystalline order of the glasses which is totally differed from that of cerium free glass, since amorphous character is the dominant.

Cite this paper

El-Damrawi, G. and Behairy, A. (2018) Structural Role of Cerium Oxide in Lead Silicate Glasses and Glass Ceramics. Journal of Minerals and Materials Characterization and Engineering, 6, 438-447.


  1. 1. Akasaka, Y., Yasui, I. and Nanba, T. (1993) Network Structure of RO2-2B2O3 Glasses. Physics and Chemistry of Glasses, 34, 232-237.

  2. 2. Iwadate, Y., Hattori, T., Nishiyama, S., Fukushima, K., Igawa, N. and Noda, K. (1996) Short-Range Structural Analysis of an Oxide Glass Composed of Light and Heavy Elements: 3B2O3-2PbO Glass by X-Ray Diffraction. Journal of Materials Science Letters, 15, 776-780.

  3. 3. Takaishi, T., Jin, J., Uchino, T. and Yoko, T. (2000) Structural Study of PbO-B2O3 Glasses by X-Ray Diffraction and 11B MAS NMR Techniques. Journal of the American Ceramic Society, 83, 2543-2548.

  4. 4. Fayon, F., Bessada, C., Massiot, D., Farnan, I. and Coutures, J.P. (1998) 29Si and 207PbNMR Study of Local Order in Lead Silicate Glasses. Journal of Non-Crystalline Solids, 232-234, 403-408.

  5. 5. Imaoka, M., Hasegawa, H. and Yasui, I. (1986) X-ray Diffraction Analysis on the Structure of the Glasses in the System PbO-SiO2. Journal of Non-Crystalline Solids, 85, 393-412.

  6. 6. El-Damrawi, G. and Gharghar, F. (2017) Magnetic Properties of xCeO2·(50-x) PbO·50B2O3 Glasses and Glass Ceramics. Journal of Advances in Physics, 13, 4486-449.

  7. 7. El-Damrawi, G., Gharghar, F. and Ramadan, R. (2016) Structural Studies on New xCeO2·(50-x)PbO·50B2O3 Glasses and Glass Ceramics. Journal of Non-Crystalline Solids, 452, 291-296.

  8. 8. Walkey, C., Das, S., Seal, S., Erlichman, J., Heckman, K., Ghibelli, L., James, E., McGinnis, F. and Self, W.T. (2015) Catalytic Properties and Biomedical Applications of Cerium Oxide Nanoparticles. Environmental Science: Nano, No. 1.

  9. 9. Deliormanli, A.M. (2015) Synthesis and Characterization of Cerium- and Gallium-Containing Borate Bioactive Glass Scaffolds for Bone Tissue Engineering, Journal of Materials Science: Materials in Medicine, 26, 67.

  10. 10. Salinas, A.J., Shruti, S., Malavasi, G., Menabue, L. and Vallet-Regí, M. (2011) Substitutions of Cerium, Gallium and Zinc in Ordered Mesoporous Bioactive Glasses. Acta Biomaterialia, 7, 3452-3458.

  11. 11. Biochem, C. (2006) Cerium and Yttrium Oxide Nanoparticles Are Neuroprotective. Biochemical and Biophysical Research Communications, 342, 86-91,

  12. 12. Das, M., Patil, S., Bhargava, N., Kang, J.-F., Riedel, L.M., Seal, S. and Hickman, J.J. (2007) Auto-Catalytic Ceria Nanoparticles Offer Neuroprotection to Adult Rat Spinal Cord Neurons. Biomaterials, 28, 1918-1925.

  13. 13. Kaur, A., Khanna, A., Singla, S., Dixit, A., Kothiyal, G.P., Krishnan, K., Aggarwal, S.K., Sathe, V., González, F. and González-Barriuso, M. (2013) Structure-Property Correlations in Lead Silicate Glasses and Crystalline Phases. Phase Transitions, 86, 759-777.

  14. 14. Furukawa, T., Fox, K.E. and White, W.B. (1981) Raman Spectroscopic Investigation of the Structure of Silicate Glasses. III. Raman Intensities and Structural Units in Sodium Silicate Glasses. The Journal of Chemical Physics, 75, Article ID: 3226e3237.

  15. 15. Shrikhande, K.V., Sudarsan, V., Kothiyat, P.G. and Kulshreshtha, K.S. (2001) 29Si MAS NMR and Microhardness Studies of Some Lead Silicate Glasses with and without Modifiers. Journal of Non-Crystalline Solids, 283, 18.

  16. 16. Choi, W.C., Lee, H.N., Kim, E.K., Kim, Y., Park, C.-Y., Kim, H.S. and Lee, J.Y. (1999) Violet/Blue Light-Emitting Cerium Silicates. Applied Physics Letters, 75, 2389-2391.

  17. 17. Wang, Z. and Cheng, L. (2015) Structural Features and Synthesis of CeO2-Doped Boroaluminosilicate Oxyfluoride Transparent Glass Ceramics. Journal of Chemistry, 2015, 1-10.

  18. 18. Culea, E., Pop, L. and Bosca, M. (2010) Structural and Physical Characteristics of CeO2-GeO2-PbO Glasses and Glass Ceramics. Journal of Alloys and Compound, 505, 754-757.

  19. 19. El Damrawi, G., Müller-Warmuth, W., Doweidar, H. and Gohar, A. (1992) Structure and Heat Treatment Effects of Sodium Borosilicate Glasses as Studied by 29Si and 11B NMR. Journal of Non-Crystalline Solids, 146, 137-144.

  20. 20. El-Damrawi, G., Müller-Warmuth, W., Doweidar, H. and Gohar, I.A. (1993) 29Si and 27Al Nuclear Magnetic Resonance Studies of Na2O-Al2O3-B2O3-SiO2 Glasses. Physics and Chemistry of Glasses, 34, 52-57.

  21. 21. Eldamrawi, G., Hassan, A.K., Kamal, H., Aboelez, M. and Labeeb, S. (2016) Structural Investigations on Na2O-CaO-V2O5-SiO2 Bioglass Ceramics. British Journal of Applied Science & Technology, 16, 1-9.

  22. 22. El-Damrawi, G., Doweidar, H. and Kamal, H. (2014) Characterization of New Categories of Bioactive Based Tellurite and Silicate Glasses. Silicon, 9, 503-509.

  23. 23. El-Damrawi, G., Doweidar, H. and Kamal, H. (2013) Structure and Crystallization Behavior of Silicate-Based Bioactive Glass Ceramics. Australian Journal of Basic and Applied Sciences, 7, 573-583.