Mixed Alkaline Effect in Antimony-Based Glasses
- Autores: Kubliha M.1, Maache D.2, Bosak O.1, Minarik S.1, Trnovcova V.3, Lukic-Petrovic S.4, Soltani M.T.2
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							Afiliações: 
							- Faculty of Materials Science and Technology, Slovak University of Technology
- Laboratoire de physique photonique et nanomatériaux multifonctionnels, University of Biskra
- University of Constantin the Philosopher in Nitra, Department of Physics
- University of Novi Sad, Faculty of Science, Department of Physics
 
- Edição: Volume 55, Nº 6 (2019)
- Páginas: 510-516
- Seção: Article
- URL: https://journals.rcsi.science/1023-1935/article/view/190531
- DOI: https://doi.org/10.1134/S1023193519060119
- ID: 190531
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Resumo
The mixed alkaline effect (MAE) is a well-known anomaly in glasses. It results in a non-linear response of various physical properties on mixing of alkali ions in the glass. In this paper, the MAE is studied in antimony oxides based glasses 60Sb2O3–20MoO3–(20 – x)Li2O–xNa2O and 60Sb2O3–20MoO3–(20 – x)Li2O–xK2O (in mol %). The influence of Na/Li and K/Li ratios on ionic AC and DC conductivities, and Tg is presented. Dependences of Tg on x, in both types of glasses, have typical minima at x ≅ 10, it means that the minima take place at approximately equal concentrations of both mixed alkali ions. The minimum for K2O containing glasses is deeper, probably due to a larger difference between ionic radii of K+ and Li+ ions. In glasses with one type of alkali ion, Tg decreases in the sequence: K → Li → Na. Temperature dependences of the DC conductivity obey Arrhenius-like relation. The conductivity steeply decreases with increasing Na or K content due to the larger ionic radius of both ions comparing to that of Li ions. At the same time, the conduction activation energy goes through a flat maximum at x = 15 (1.21 eV) for Na2O modifier and at x = 5 (1.16 eV), for K2O modifier. In antimony oxide based glasses, Li+, Na+, and K+ ions are modifiers and dominant charge-carriers. Due to larger ionic radii of Na+, and K+, the decrease of the conductivity after their addition is reasonable.
Sobre autores
M. Kubliha
Faculty of Materials Science and Technology, Slovak University of Technology
														Email: ondrej.bosak@stuba.sk
				                					                																			                												                	Eslováquia, 							Trnava, 91724						
D. Maache
Laboratoire de physique photonique et nanomatériaux multifonctionnels, University of Biskra
														Email: ondrej.bosak@stuba.sk
				                					                																			                												                	Argélia, 							Biskra, BP 145						
O. Bosak
Faculty of Materials Science and Technology, Slovak University of Technology
							Autor responsável pela correspondência
							Email: ondrej.bosak@stuba.sk
				                					                																			                												                	Eslováquia, 							Trnava, 91724						
S. Minarik
Faculty of Materials Science and Technology, Slovak University of Technology
														Email: ondrej.bosak@stuba.sk
				                					                																			                												                	Eslováquia, 							Trnava, 91724						
V. Trnovcova
University of Constantin the Philosopher in Nitra, Department of Physics
														Email: ondrej.bosak@stuba.sk
				                					                																			                												                	Eslováquia, 							Nitra, 94974						
S. Lukic-Petrovic
University of Novi Sad, Faculty of Science, Department of Physics
														Email: ondrej.bosak@stuba.sk
				                					                																			                												                	Sérvia, 							Novi Sad, 21000						
M. Soltani
Laboratoire de physique photonique et nanomatériaux multifonctionnels, University of Biskra
														Email: ondrej.bosak@stuba.sk
				                					                																			                												                	Argélia, 							Biskra, BP 145						
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