Glasses having the composition, [(70-x) mol% B2O3- x mol% Bi2O3- 10 mol% BaO- 20 mol% Na2O, where 0≤ x ≤20], have been prepared by the melt quenching method. Density, molar volume, infrared analysis, optical parameters and Electrical properties have been thoroughly investigated. It was found that, both density and molar volume increased with the gradual replacement of B2O3 by Bi2O3 and the comparison between their experimental and empirical values confirm the amorphous nature and the random structure of all samples. The obtained infrared results indicated that different structural borate groups appeared such as BO4 units (in di-, tri- and penta-borate groups) and BO3 units (in meta- and ortho-borate chains). Also, both BiO3 and BiO6 are present in all Bi doped glasses, and the BiO3 / BiO6 ratio appeared to be approximately stable as Bi2O3 was increased to 15 mol%, then it showed a jump increase when BiO3 reached 20 mol%. The optical band gap energy and cut-off wavelength increased with the increase of Bi2O3 while Urbach energy decreased. On the other hand, the electrical conductivity decreased as Bi2O3 was gradually replaced by B2O3, while the activation energy increased and all samples exhibit semi-conductors behavior and the values of the exponent factor decreased gradually with temperature, which is compatible with the correlated barrier hopping conduction mechanism.
Published in | American Journal of Aerospace Engineering (Volume 5, Issue 1) |
DOI | 10.11648/j.ajae.20180501.11 |
Page(s) | 1-8 |
Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
Copyright |
Copyright © The Author(s), 2018. Published by Science Publishing Group |
Sodium-Borate Glasses, FTIR, Optical Parameters, AC Conductivity
[1] | J. E. Shelby, Introduction to Glass Science and Technology, The Royal Society of Chemis try, UK, (1997). |
[2] | S. Sanghi, S. Duhan, A. Agarwal and P. Aghamkar, J. Alloys and Compounds, 488 (2009) 458. |
[3] | N. A. Eissa, A. M. Sanad, A. A. El-Saghier, H. A. Sallam and A. G. Mostafa, Acta Physica Hungarica, 59 (1986) 297. |
[4] | Krough-Moe, J. Phys. Chem. Glasses, 6 (1965) 46. |
[5] | T. Nishida, M. SuzuKi, S. Kubuki, M. Katata and Y. Maeda, J. Non Cryst. Solids, 194 (1996) 23. |
[6] | A. Varshneya, "Fundamentals of Inorganic Glasses", Academic Press Inc., New-York, (1994). |
[7] | T. Yano, N. Kunimine, S. Shibata and M. Yamane, J. Non-Cryst. Solids, 321 (2003) 137. |
[8] | T. Yano, N. Kunimine, S. Shibata and M. Yamane, J. Non-Cryst. Solids, 321 (2003) 157. |
[9] | I. Oprea, PhD thesis, Physics Dep., Osnabruck Univ., "Optical Properties of Borate Glass-Ceramics", (2005). |
[10] | Kulwinder Kaur, K. J. Singh and Vikas Anand, J. Radiation Physics and Chemistry, 120 (2016) 72. |
[11] | H. El Mkami, J. Phys. Chem. Solids, 61 (2000) 153. |
[12] | G. S. M. Ahmed, A. S. Mahmoud, S. M. Salem and T. Z. Abo-Elnasr, American J. Phys. & Applications, 3, 4 (2015) 112. |
[13] | H. A. Saudi, A. Abd-Elalim, T. Z. Abo-Elnasr and A. G. Mostafa, Nature & Science, 13 (2015) 71. |
[14] | S. A. MacDonald, C. R. Schardt, D. J. Masiello and J. H. Simmons, J. Non-Cryst. Solids, 275 (2000) 72. |
[15] | A. A. Akatov, B. S. Nikonov, B. I. Omelyanenko, S. V. Stefanovsky and J. C. Marra, Phys. Chem. Glasses, 35 (2009) 245. |
[16] | M. S. Aziz, F. Abdel-Wahab, A. G. Mostafa and E. M. El Agwany, J. Mater. Chem. Phys., 91 (2005) 532. |
[17] | A. Radu, L. Baia, W. Kiefer and S. Simon, J. Vibrational Spectroscopy, 39 (2005) 130. |
[18] | M. A. Marzouk, F. H. El-Batal, W. H. Eisa and N. A. Ghoneima, J. Non-Crystalline Solids, 387 (2014) 155. |
[19] | Ravneet Kaur, Surinder Singh and O. P. Pandey, J. Molecular Structure, 1049 (2013) 409. |
[20] | T. D. AbdelAziz, F. M. Ezz El-Din, H. A. El Batal and A. M. Abdelghany, J. Spectrochimica Acta Part A, (Molecular and Biomolecular Spectroscopy), 131 (2014) 501. |
[21] | P. Limkitjaroenporn, J. Kaewkhao, P. Limsuwan and W. Chewpraditkul, J. Physics and Chemistry of Solids, 72 (2011) 245. |
[22] | L. Baia, R. Stefan, J. Popp, S. Simon and W. Kiefer, J. Non-Cryst. Solids, 324 (2003) 109. |
[23] | R. Iordanova, V. Dimitrov, Y. Dimitriev and D. Klissurski, J. Non-Cryst. Solids, 180 (1994) 58. |
[24] | S. Shailajha, K. Geetha, P. Vasantharani and S. P. Sheik Abdul Kadhar, J. Spectrochimica Acta Part A, (Molecular and Biomolecular Spectroscopy), 138 (2015) 846. |
[25] | Yasser B. Saddeek and M. S. Gaafar, J. Materials Chemistry and Physics, 115 (2009) 280. |
[26] | A. M. Abdel-Ghany, A. A. Bendary, T. Z. Abou-Elnasr, M. Y. Hassaan and A. G. Mostafa, J. Nature and Science, 12 (8) (2014) 153. |
[27] | N. F. Mott, E. A. Davis, '' Electronic processes in Non-Crystalline Materials '', Clarendon, Oxford, (1979). |
[28] | TG. VM. Rao, AR. Kumar and MR. Reddy, J. Non-Cryst. Solids, 356 (2012) 25. |
[29] | CM. Kramjce, IP. Studenyak and MV. Kurik, J. Non-Cryst. Solids, 355 (2009) 54. |
[30] | M. Zanini and J. Tauc, J. Non-Cryst. Solids, 23 (1977) 349. |
[31] | A. Agarwal, V. P. Seth, S. Sanghi, P. S. Gahlot, and D. R. Goyal, Radiation Effects & Defects in Solids, 158 (2003) 793. |
[32] | Ch. Rajasree and Rao. D. Krishna, J. Non-Cryst. Solids, 357 (2011) 836. |
[33] | S. R. Elliott, adv. Phys., 18 (1987) 41. |
[34] | S. R. Elliott, adv. Phys., 36 (2) (1987) 135. |
[35] | V. C. Veeranna Gowda and R. V. Anavenka, Solid Stat. Ionics, 176 (2005) 1393. |
[36] | G. Little Flower, G. Sahaya Baskaran, M. Srinivasa Reddy and N. Veeraiah, J. Physica B, 393 (2007) 72. |
[37] | D. E. Day, J. Non-Cryst. Solids, 21 (1976) 343. |
[38] | E. Mansour, J. Physica B, 362 (2005) 88. |
[39] | J. C. Giantini and J. V. Zancheha, J. Non-Cryst. Solids, 34 (1979) 419. |
APA Style
Sayed M. Salem, Taha Z. Abou-Elnasr, Wael A. El-Gammal, Ahmed S. Mahmoud, Heba A. Saudi, et al. (2018). Optical Parameters and Electrical Transport Properties of Some Barium-Sodium-Borate Glasses Doped Bismuth Oxide. American Journal of Aerospace Engineering, 5(1), 1-8. https://doi.org/10.11648/j.ajae.20180501.11
ACS Style
Sayed M. Salem; Taha Z. Abou-Elnasr; Wael A. El-Gammal; Ahmed S. Mahmoud; Heba A. Saudi, et al. Optical Parameters and Electrical Transport Properties of Some Barium-Sodium-Borate Glasses Doped Bismuth Oxide. Am. J. Aerosp. Eng. 2018, 5(1), 1-8. doi: 10.11648/j.ajae.20180501.11
AMA Style
Sayed M. Salem, Taha Z. Abou-Elnasr, Wael A. El-Gammal, Ahmed S. Mahmoud, Heba A. Saudi, et al. Optical Parameters and Electrical Transport Properties of Some Barium-Sodium-Borate Glasses Doped Bismuth Oxide. Am J Aerosp Eng. 2018;5(1):1-8. doi: 10.11648/j.ajae.20180501.11
@article{10.11648/j.ajae.20180501.11, author = {Sayed M. Salem and Taha Z. Abou-Elnasr and Wael A. El-Gammal and Ahmed S. Mahmoud and Heba A. Saudi and Ahmed G. Mostafa}, title = {Optical Parameters and Electrical Transport Properties of Some Barium-Sodium-Borate Glasses Doped Bismuth Oxide}, journal = {American Journal of Aerospace Engineering}, volume = {5}, number = {1}, pages = {1-8}, doi = {10.11648/j.ajae.20180501.11}, url = {https://doi.org/10.11648/j.ajae.20180501.11}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajae.20180501.11}, abstract = {Glasses having the composition, [(70-x) mol% B2O3- x mol% Bi2O3- 10 mol% BaO- 20 mol% Na2O, where 0≤ x ≤20], have been prepared by the melt quenching method. Density, molar volume, infrared analysis, optical parameters and Electrical properties have been thoroughly investigated. It was found that, both density and molar volume increased with the gradual replacement of B2O3 by Bi2O3 and the comparison between their experimental and empirical values confirm the amorphous nature and the random structure of all samples. The obtained infrared results indicated that different structural borate groups appeared such as BO4 units (in di-, tri- and penta-borate groups) and BO3 units (in meta- and ortho-borate chains). Also, both BiO3 and BiO6 are present in all Bi doped glasses, and the BiO3 / BiO6 ratio appeared to be approximately stable as Bi2O3 was increased to 15 mol%, then it showed a jump increase when BiO3 reached 20 mol%. The optical band gap energy and cut-off wavelength increased with the increase of Bi2O3 while Urbach energy decreased. On the other hand, the electrical conductivity decreased as Bi2O3 was gradually replaced by B2O3, while the activation energy increased and all samples exhibit semi-conductors behavior and the values of the exponent factor decreased gradually with temperature, which is compatible with the correlated barrier hopping conduction mechanism.}, year = {2018} }
TY - JOUR T1 - Optical Parameters and Electrical Transport Properties of Some Barium-Sodium-Borate Glasses Doped Bismuth Oxide AU - Sayed M. Salem AU - Taha Z. Abou-Elnasr AU - Wael A. El-Gammal AU - Ahmed S. Mahmoud AU - Heba A. Saudi AU - Ahmed G. Mostafa Y1 - 2018/02/07 PY - 2018 N1 - https://doi.org/10.11648/j.ajae.20180501.11 DO - 10.11648/j.ajae.20180501.11 T2 - American Journal of Aerospace Engineering JF - American Journal of Aerospace Engineering JO - American Journal of Aerospace Engineering SP - 1 EP - 8 PB - Science Publishing Group SN - 2376-4821 UR - https://doi.org/10.11648/j.ajae.20180501.11 AB - Glasses having the composition, [(70-x) mol% B2O3- x mol% Bi2O3- 10 mol% BaO- 20 mol% Na2O, where 0≤ x ≤20], have been prepared by the melt quenching method. Density, molar volume, infrared analysis, optical parameters and Electrical properties have been thoroughly investigated. It was found that, both density and molar volume increased with the gradual replacement of B2O3 by Bi2O3 and the comparison between their experimental and empirical values confirm the amorphous nature and the random structure of all samples. The obtained infrared results indicated that different structural borate groups appeared such as BO4 units (in di-, tri- and penta-borate groups) and BO3 units (in meta- and ortho-borate chains). Also, both BiO3 and BiO6 are present in all Bi doped glasses, and the BiO3 / BiO6 ratio appeared to be approximately stable as Bi2O3 was increased to 15 mol%, then it showed a jump increase when BiO3 reached 20 mol%. The optical band gap energy and cut-off wavelength increased with the increase of Bi2O3 while Urbach energy decreased. On the other hand, the electrical conductivity decreased as Bi2O3 was gradually replaced by B2O3, while the activation energy increased and all samples exhibit semi-conductors behavior and the values of the exponent factor decreased gradually with temperature, which is compatible with the correlated barrier hopping conduction mechanism. VL - 5 IS - 1 ER -