Abstract:Please cite this article in press as: Sujatha B, et al. Electronic and ionic conductivity studies on microwave synthesized glasses containing transition metal ions. J Mater Res Technol. 2016. http://dx.
“…On the other hand, glasses which exhibit significant contribution of polaronic conduction along with the ionic one show two semicircles in the impedance plot, Figure 5B. 22,[29][30][31][32][33] In our study we applied gold electrodes for electrical measurements which are blocking for ions and non-blocking for polarons. 22,[29][30][31][32][33] In our study we applied gold electrodes for electrical measurements which are blocking for ions and non-blocking for polarons.…”
Section: Electrical Transportmentioning
confidence: 91%
“…Four series of glasses in the quaternary systems: 10,20,30,40,50, 60 (mol%) B) xWO 3 -(30À0.5x)Na 2 O-(30À0.5x)ZnO-40P 2 O 5 , with x = 0, 10, 20, 30, 40, 50, 60 (mol%) 10,20,30,40,50, 60 (mol%) 10, 20, 30, 40, 50, 60 (mol%).…”
Section: Methodsmentioning
confidence: 99%
“…Such a behavior is found to be typical for mixed conduction in various materials where selectively blocking electrodes (e.g., blocking for one carrier and non-blocking for the other one) are used. 22,[29][30][31][32][33] In our study we applied gold electrodes for electrical measurements which are blocking for ions and non-blocking for polarons. Therefore, the high frequency semicircle observed for Na-50W glass is associated with the dielectric relaxation of the bulk, whereas the additional semicircle at lower frequencies refers to a chemical relaxation due to unblocked polaronic diffusion.…”
Transformation of electrical transport from ionic to polaronic in glasses, which are a potential class of new cathode materials, has been investigated in four series containing WO3/MoO3 and Li+/Na+ ions, namely: xWO3–(30−0.5x)Li2O–(30−0.5x)ZnO–40P2O5, xWO3–(30−0.5x)Na2O–(30.5x)ZnO–40P2O5, xMoO3–(30−0.5x)Li2O–(30−0.5x)ZnO–40P2O5, and xMoO3–(30−0.5x)Na2O–(30−0.5x)ZnO–40P2O5, 0 ≤ x ≤ 60, (mol%). This study reports a detailed analysis of the role of structural modifications and its implications on the origin of electrical transport in these mixed ionic‐polaron glasses. Raman spectra show the clustering of WO6 units by the formation of W–O–W bonds in glasses with high WO3 content while the coexistence of MoO4 and MoO6 units is evidenced in glasses containing MoO3 with no clustering of MoO6 octahedra. Consequently, DC conductivity of tungstate glasses with either Li+ or Na+ exhibits a transition from ionic to polaronic showing a minimum at about 20‐30 mol% of WO3 as a result of ion‐polaron interactions followed by a sharp increase for six orders of magnitude as WO3 content increases. The formation of WO6 clusters involved in W‐O‐W linkages for tungsten glasses plays a key role in significant increase in DC conductivity. On the other hand, DC conductivity is almost constant for glasses containing MoO3 suggesting an independent ionic and polaronic transport pathways for glasses containing 10‐50 mol% of MoO3.
“…On the other hand, glasses which exhibit significant contribution of polaronic conduction along with the ionic one show two semicircles in the impedance plot, Figure 5B. 22,[29][30][31][32][33] In our study we applied gold electrodes for electrical measurements which are blocking for ions and non-blocking for polarons. 22,[29][30][31][32][33] In our study we applied gold electrodes for electrical measurements which are blocking for ions and non-blocking for polarons.…”
Section: Electrical Transportmentioning
confidence: 91%
“…Four series of glasses in the quaternary systems: 10,20,30,40,50, 60 (mol%) B) xWO 3 -(30À0.5x)Na 2 O-(30À0.5x)ZnO-40P 2 O 5 , with x = 0, 10, 20, 30, 40, 50, 60 (mol%) 10,20,30,40,50, 60 (mol%) 10, 20, 30, 40, 50, 60 (mol%).…”
Section: Methodsmentioning
confidence: 99%
“…Such a behavior is found to be typical for mixed conduction in various materials where selectively blocking electrodes (e.g., blocking for one carrier and non-blocking for the other one) are used. 22,[29][30][31][32][33] In our study we applied gold electrodes for electrical measurements which are blocking for ions and non-blocking for polarons. Therefore, the high frequency semicircle observed for Na-50W glass is associated with the dielectric relaxation of the bulk, whereas the additional semicircle at lower frequencies refers to a chemical relaxation due to unblocked polaronic diffusion.…”
Transformation of electrical transport from ionic to polaronic in glasses, which are a potential class of new cathode materials, has been investigated in four series containing WO3/MoO3 and Li+/Na+ ions, namely: xWO3–(30−0.5x)Li2O–(30−0.5x)ZnO–40P2O5, xWO3–(30−0.5x)Na2O–(30.5x)ZnO–40P2O5, xMoO3–(30−0.5x)Li2O–(30−0.5x)ZnO–40P2O5, and xMoO3–(30−0.5x)Na2O–(30−0.5x)ZnO–40P2O5, 0 ≤ x ≤ 60, (mol%). This study reports a detailed analysis of the role of structural modifications and its implications on the origin of electrical transport in these mixed ionic‐polaron glasses. Raman spectra show the clustering of WO6 units by the formation of W–O–W bonds in glasses with high WO3 content while the coexistence of MoO4 and MoO6 units is evidenced in glasses containing MoO3 with no clustering of MoO6 octahedra. Consequently, DC conductivity of tungstate glasses with either Li+ or Na+ exhibits a transition from ionic to polaronic showing a minimum at about 20‐30 mol% of WO3 as a result of ion‐polaron interactions followed by a sharp increase for six orders of magnitude as WO3 content increases. The formation of WO6 clusters involved in W‐O‐W linkages for tungsten glasses plays a key role in significant increase in DC conductivity. On the other hand, DC conductivity is almost constant for glasses containing MoO3 suggesting an independent ionic and polaronic transport pathways for glasses containing 10‐50 mol% of MoO3.
“…Multicomponent glasses containing TMO (V 2 O 5 , Fe 2 O 3 , CuO, MoO 3 , WO 3 , etc), glass former (B 2 O 3 , P 2 O 5 , TeO 2 , etc), and alkali oxides as modifiers (Li 2 O, Na 2 O, etc) have been extensively reviewed . These glasses are known to be mixed ionic‐electronic conductors .…”
Section: Introductionmentioning
confidence: 99%
“…Multicomponent glasses containing TMO (V 2 O 5 , Fe 2 O 3 , CuO, MoO 3 , WO 3 , etc), glass former (B 2 O 3 , P 2 O 5 , TeO 2 , etc), and alkali oxides as modifiers (Li 2 O, Na 2 O, etc) have been extensively reviewed. [9][10][11][12] These glasses are known to be mixed ionic-electronic conductors. 10,11 It was found that alkali-free oxide glasses 13,14 in the TeO 2 -V 2 O 5 -MoO 3 and V 2 O 5 -Sb-TeO 2 systems 15 have nonohmic conduction leading to negative resistance/switching phenomenon at high electric fields.…”
Summary
The ac conductivity of 70WO3–30P2O5 glass composition prepared by melt quenching was first studied in the temperature range 25°C to 350°C. The conductivity of the semiconducting glass is investigated with various electrodes (Pt and Ga‐Ag alloy). It is shown that the type of spectrum of cell impedance depends on the chosen electrodes. The influence of the samples geometry on the conduction is established. The influence of gas atmosphere (argon, oxygen, and air of different humidity) on electrical conductivity of tungsten‐phosphate glass on is studied for the first time. A mixed electronic‐ionic conductivity in the 70WO3–30P2O5 glass is found out. The transport numbers are shown as a function of temperature. Ionic and electronic contribution to the conduction is estimated. The electrical conductivity of glass undergoes changes from 8.6 × 10−8 (25°C) to 3.1 × 10−4 S/cm (300°C) in air.
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