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Journal articles on the topic 'Electron Conducting Glasses'

Author: Grafiati
Published: 7 September 2023

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1

Hibbert, D. B., T. M. Roberts, and S. H. Bhote. "A model of field induced electron emission from ionically-conducting glasses." Journal of Physics D: Applied Physics 18, no. 9 (September 14, 1985): 1833–42. http://dx.doi.org/10.1088/0022-3727/18/9/014.

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2

Leslie‐Pelecky, D. L., F. VanWijland, C. N. Hoff, J. A. Cowen, A. Gavrin, and C. ‐L Chien. "Comparison of the electron‐spin‐resonance linewidth in multilayered CuMn spin glasses with insulating versus conducting interlayers." Journal of Applied Physics 75, no. 10 (May 15, 1994): 6489–91. http://dx.doi.org/10.1063/1.356973.

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3

Frąckiewicz, Justyna E., and Tomasz K. Pietrzak. "Highly Conducting Li(Fe1−xMnx)0.88V0.08PO4 Cathode Materials Nanocrystallized from the Glassy State (x = 0.25, 0.5, 0.75)." Materials 14, no. 21 (October 27, 2021): 6434. http://dx.doi.org/10.3390/ma14216434.

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This study showed that thermal nanocrystallization of glassy analogs of LiFe1−xMnxPO4 (with the addition of vanadium for improvement of glass forming properties) resulted in highly conducting materials that may be used as cathodes for Li-ion batteries. The glasses and nanomaterials were studied with differential thermal analysis, X-ray diffractometry, and impedance spectroscopy. The electrical conductivity of the nanocrystalline samples varied, depending on the composition. For x=0.5, it exceeded 10−3 S/cm at room temperature with an activation energy as low as 0.15 eV. The giant and irreversible increase in the conductivity was explained on the basis of Mott’s theory of electron hopping and a core-shell concept. Electrochemical performance of the active material with x=0.5 was also reported.
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4

Ren, Yang, Gao Yang Zhao, and Jie Shen. "Preparation of Fluorine Doped Tin Oxide Film by Ultrasonic Spray Pyrolysis." Materials Science Forum 695 (July 2011): 594–97. http://dx.doi.org/10.4028/www.scientific.net/msf.695.594.

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Fluorine doped tin oxide (FTO) film is one of the most promising transparent conducting materials. It can be used for Low-E glasses, thin film solar cells, displays, etc. FTO film can be fabricated by various techniques. The technique of sol-gel combined with ultrasonic spray pyrolysis gives the possibility to produce high-quality large-scale FTO films. In this paper, the FTO sol is successfully prepared using pentahydrate stannic chloride (SnCl4•5H2O), hydrogen fluoride (HF) and methanol. Using the FTO sol, FTO films are prepared by ultrasonic spray pyrolysis technique. X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), scanning electron microscopy (SEM), and atomic force microscopy (AFM) are used to characterize the FTO films coated on glass substrates. Results indicate that the as-deposited films are polycrystalline SnO2 phase with tetragonal crystal structure, and that the average grain size for the samples is 160nm. The optical and electrical properties of the FTO film are also analyzed.
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5

Kordas, G., R. A. Weeks, and D. L. Kinser. "Paramagnetic conduction electrons in GeSx-glasses." Journal of Non-Crystalline Solids 71, no. 1-3 (May 1985): 157–61. http://dx.doi.org/10.1016/0022-3093(85)90284-4.

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6

Amir, Ariel. "Universal frequency-dependent conduction of electron glasses." EPL (Europhysics Letters) 107, no. 4 (August 1, 2014): 47011. http://dx.doi.org/10.1209/0295-5075/107/47011.

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7

Mandal, S., and S. Hazra. "Structural and physical properties of Fe2O3-doped lead vanadate glass." Journal of Materials Research 15, no. 1 (January 2000): 218–21. http://dx.doi.org/10.1557/jmr.2000.0035.

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The role of Fe2O3in the structural and physical properties of ternary lead vanadium iron glass system has been studied in comparison with the binary lead vanadate glasses. X-ray diffraction, scanning electron microscopy, and differential thermal analysis show that homogeneous glasses of composition 10Fe2O3 · xV2O5 · (90 − x)PbO can be obtained for x = 50 to 80 mol%. Observation from the infrared spectroscopy shows that the basic building blocks of these glasses are same as those of crystalline V2O5, while differential thermal analysis and electrical conduction of these glasses suggest that there is a strong role of iron, both in the glass network and in the conduction mechanism for the glasses containing a low percentage of vanadium.
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8

Rossiter, PL. "Conduction Electron Scattering in Alloys." Australian Journal of Physics 39, no. 4 (1986): 529. http://dx.doi.org/10.1071/ph860529.

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The aim of this review is to present a simple physical picture which shows how the electrical resistivity of a system depends upon the spatial extent and lifetime of the scattering disturbance measured in relation to the conduction electron mean free path and relaxation time. The contribution from spin fluctuations associated with isolated magnetic impurities is discussed on the basis of this model and it is shown that at temperatures below the characteristic spin fluctuation temperature the impurity acts as though it were nonmagnetic. Some results are given for both 'Kondo' (Anderson) and exchange enhanced (Wolfi) systems. Spin glasses are also discussed and the resistivity behaviour is shown to result from a competition between the RKKY interaction and spin fluctuation effects. Ordered magnetic clusters are shown to be static for periods comparable with the conduction electron relaxation time, so that there is no resistivity anomaly expected at the superparamagnetic blocking temperature. The observed temperature dependence of the resistivity then follows simply from the change in magnetic correlations within the cluster.
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9

Spencer, Jacob N., Andrea Folli, Hong Ren, and Damien M. Murphy. "An EPR investigation of defect structure and electron transfer mechanism in mixed-conductive LiBO2–V2O5 glasses." Journal of Materials Chemistry A 9, no. 31 (2021): 16917–27. http://dx.doi.org/10.1039/d1ta02352g.

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A series of LiBO2–V2O5 glasses of varying contents were investigated using Electron Paramagnetic Resonance (EPR) spectroscopy. This approach provides a convenient method to rationalise the defect structure and electron transfer mechanism.
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10

Jun, Liu, J. Portier, B. Tanguy, J. J. Videau, M. Ait Allal, J. Morcos, and J. Salardenne. "Application of Silver Conducting Glasses to Solid State Batteries and Sensors." Active and Passive Electronic Components 14, no. 2 (1990): 81–94. http://dx.doi.org/10.1155/1990/82403.

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Fast silver ion conducting glasses as electrochemical devices have been tested. A silver iodine battery using a silver ionic conducting glass (AgPO3-Ag2S-AgI) has been studied. The interaction of some gases (O2CI2, H2S) with the electrochemical chains: Pt/Sb2S3-AgI (glass)/Ag and Pt/AgCl (thin film)/Sb2S3- AgI (glass)/Ag has been investigated. Finally, the behavior of thin films of Ag2S3-Ag2S-CdS glasses as sensitive membranes for Cd detection in solution has been tested on MIS structures Au/Si/SiO2/ Membrane/Cd in solution/Reference electrode.
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11

El Damrawi, G., A. M. Abdelghany, and H. Salaheldin. "Effect of aluminum oxide on the structure and conduction behaviors of silver borate glasses." Bulletin of the Chemical Society of Ethiopia 36, no. 3 (July 15, 2022): 597–606. http://dx.doi.org/10.4314/bcse.v36i3.9.

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ABSTRACT. The current study focuses on glass preparation and characterization in the glass system of chemical formula xAl2O3 (35-x) Ag2O.65B2O3 (0≤x≤35 mol%), where Ag2O is replaced with Al2O3. To examine a wide range of both structure and morphology of the prepared glasses, nuclear magnetic resonance (NMR) of 27Al nuclei, X-ray diffraction (XRD) spectroscopy, and transmission electron microscopy (TEM) are used. In Al2O3-rich glass, the well-formed AlO6, AlO5, and AlO4 structural groups are the well-formed units. In samples of (20 and 30 mol % Al2O3), tetrahedral AlO4 and traces from AlO6 units could be detected. At lower concentrations of Al2O3 (10 mol%), the dominant forming unit is only AlO4 groups containing non-bridging oxygen bonds (NBO). The XRD spectra confirm the amorphous nature of the glasses of Al2O3 ˂20 mol% while glasses of higher Al2O3 concentrations contain crystalline Ag2Al2B2O7 formed due to the higher oxygen packaging of the mixed AlO5 and AlO4 compared with that of glasses containing only AlO4 species only. The morphology of crystalline units is confirmed from TEM to differ from that of an amorphous composition. The increase of activation energy and the hardness number of the glasses led to an increase in the durability of the investigated glasses. KEY WORDS: Aluminum borate glass, NMR, Coordination of aluminum atom, Conductivity, Crystallization process Bull. Chem. Soc. Ethiop. 2022, 36(3), 597-606. DOI: https://dx.doi.org/10.4314/bcse.v36i3.9
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12

Sultanov, K. M., Sh A. Kuliev, and N. G. Abdullaev. "Coupled waves in conducting spin glasses." physica status solidi (b) 135, no. 1 (May 1, 1986): 163–71. http://dx.doi.org/10.1002/pssb.2221350117.

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13

Kotvitckii, Aleksandr, Galina Kraynova, Anatoly Frolov, Vitaly Ivanov, and Vladimir Plotnikov. "Structure Evolution of Fe- and Co-Based Amorphous Alloys Studied by the Electrical Resistivity Measurements." Solid State Phenomena 215 (April 2014): 185–89. http://dx.doi.org/10.4028/www.scientific.net/ssp.215.185.

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The subject of this study is the change of the electrical resistivity of Fe-based metallic glasses during heat treatment. Electrical resistivity is a structure-sensitive characteristic of materials. In metallic glasses, the scattering of conduction electrons on the disordered structure is the main mechanism responsible for the electrical resistivity. Hence amorphous metallic alloys have a much higher residual resistivity as compared to their crystalline analogs. It is typical for metallic glasses that the temperature coefficient of resistivity (TRC) is smaller than for the corresponding crystalline materials, and it can be either positive or negative.
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14

Adachi, Kenji, Sadahiro lida, and Kazuhide Hayashi. "Ruthenium clusters in lead-borosilicate glass in thick film resistors." Journal of Materials Research 9, no. 7 (July 1994): 1866–78. http://dx.doi.org/10.1557/jmr.1994.1866.

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An interparticle glass matrix in ruthenium dioxide-based thick film resistors has been studied intensively by means of analytical and high resolution transmission electron microscopy. The ruthenium dioxide phase interacts with lead-borosilicate glass at high temperature by dissolving ruthenium ions and incorporating a small number of lead and aluminum ions on the surface. Ruthenium ions diffuse through the glass network at least over a distance of 1 μm during firing, but are accommodated in the glass structure by an amount only less than 7 at. % at room temperature. High resolution electron microscopy reveals numerous ruthenium-pyrochlore crystallites in high-lead glasses, but hardly any Ru-based clusters/crystallites in low-lead glasses, where lead-rich glass clusters due to glass immiscibility and reduced lead metal clusters are more commonly observed instead of ruthenium clusters. Lead oxide is prone to reduction both in high- and low-lead glasses upon irradiating with a high-energy incident electron beam. Comparison with gold-based resistor and estimation of average dispersion length of ruthenium clusters, 2 to 4 nm, prefer the model of electron hopping via ruthenium clusters/crystallites as a dominant conduction mechanism in thick film resistors.
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15

Tanaka, K., Y. Miyamoto, M. Itoh, and E. Bychkov. "Ionic Conduction in Glasses." physica status solidi (a) 173, no. 2 (June 1999): 317–22. http://dx.doi.org/10.1002/(sici)1521-396x(199906)173:2<317::aid-pssa317>3.0.co;2-q.

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16

Minami, Tsutomu. "Recent progress in superionic conducting glasses." Journal of Non-Crystalline Solids 95-96 (December 1987): 107–18. http://dx.doi.org/10.1016/s0022-3093(87)80103-5.

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17

Abe, Yoshihiro, Mitsuhiko Hayashi, Takashi Iwamoto, Hirofumi Sumi, and L. L. Hench. "Superprotonic conducting phosphate glasses containing water." Journal of Non-Crystalline Solids 351, no. 24-26 (August 2005): 2138–41. http://dx.doi.org/10.1016/j.jnoncrysol.2005.05.010.

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18

Ingram, Malcolm D. "Relaxation processes in ionically conducting glasses." Journal of Non-Crystalline Solids 131-133 (June 1991): 955–60. http://dx.doi.org/10.1016/0022-3093(91)90708-e.

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19

Pradel, A., and M. Ribes. "Ion transport in superionic conducting glasses." Journal of Non-Crystalline Solids 172-174 (September 1994): 1315–23. http://dx.doi.org/10.1016/0022-3093(94)90658-0.

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20

Yang, Feng, Xiaoqun Zhu, Chunguang Li, Jinliang Yang, Jeffery W. Stansbury, and Jun Nie. "Electro-initiated cationic polymerization in the presence of potassium hexafluoroantimonate." RSC Adv. 4, no. 42 (2014): 22224–29. http://dx.doi.org/10.1039/c4ra02089h.

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The kinetics of electro-initiated polymerization of vinyl ethers in the presence of potassium hexafluoroantimonate are investigated by RT-FT-NIR. The apparatus for real time monitoring of the kinetics of the reaction is set up by using ITO conductive glasses. Potassium hexafluoroantimonate has been proven to be an efficient initiator for electro-initiated polymerization of vinyl ethers.
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21

Nishida, Tetsuaki, Yukimi Izutsu, Mina Fujimura, Keito Osouda, Yuki Otsuka, Shiro Kubuki, and Nobuto Oka. "Highly conductive barium iron vanadate glass containing different metal oxides." Pure and Applied Chemistry 89, no. 4 (May 24, 2017): 419–28. http://dx.doi.org/10.1515/pac-2016-0916.

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Abstract20BaO·5ZnO·5Fe2O3·70V2O5 glass annealed at 450°C for 30 min showed a marked decrease in the electric resistivity (ρ) from 4.0×105 to 4.8 Ωcm, while 20BaO·5Cu2O·5Fe2O3·70V2O5 glass from 2.0×105 to 5.0 Ωcm. As for the conduction mechanism, it proved that n-type semiconductor model in conjugation with the small polaron hopping theory was most probable. Since ZnII and CuI have a 3d10-electron configuration in the outer-most orbital, Ga2O3- and GeO2-containing vanadate glasses were explored in this study. 20BaO·5Ga2O3·5Fe2O3·70V2O5 glass showed a less remarkable decrease of ρ from 4.5×105 to 100 Ωcm, and 20BaO·5GeO2·5Fe2O3·70V2O5 glass from 3.3×106 to 400 Ωcm. Activation energies for the conduction (Ea) of GeO2- and Ga2O3-contaning glasses before the annealing were respectively estimated to be 0.42 and 0.41 eV. It proved that barium iron vanadate glass with a smaller Ea value could attain the higher conductivity after the annealing at temperaures higher than the crystalization temperature.
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22

Pradel, Annie, and Michel Ribes. "Ionically conductive chalcogenide glasses." Journal of Solid State Chemistry 96, no. 1 (January 1992): 247–57. http://dx.doi.org/10.1016/s0022-4596(05)80318-4.

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23

Pollak, M. "The electron glass: conduction, glassy dynamics and relation to other glasses." physica status solidi (c) 5, no. 3 (March 2008): 667–73. http://dx.doi.org/10.1002/pssc.200777580.

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24

Banagar, Arunkumar V., M. Prashant Kumar, N. Nagaraja, Anand Tipperudra, and Sangamesh Jakati. "DC electrical conduction in strontium vanadium borate glasses." Materials Science-Poland 38, no. 2 (June 1, 2020): 359–66. http://dx.doi.org/10.2478/msp-2020-0022.

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AbstractA series of borate glasses with the composition x(SrO)·(50 – x)V2O5·0.5(B2O3) where x = 0, 0.1, 0.2, 0.3 and 0.4 were prepared by melt-quenching technique. The non-crystalline nature of the glasses has been established by XRD studies. Room temperature density and DC electrical conductivity of the samples were investigated in the temperature range of 300 K to 443 K. The molar volume and oxygen packing density (OPD) were estimated. The results show that the density, molar volume and OPD decrease with the increasing of SrO mole fraction. The DC electrical conductivity data has been analyzed in the light of Mott’s small polaron hopping (SPH) model and the activation energies were estimated. The conductivity was observed to rapidly fall and activation energy was found to increase when SrO was incorporated into the glass network. This may indicate that Sr+ ions have not contributed to the total conductivity and the observed conductivity may be of polaronic type only, which is due to the hopping of electrons between multivalent states of vanadium. Various small polaron hopping parameters such as small polaron radius, rp, effective dielectric constant, ϵp, polaron band width, J, optical phonon frequency, υo, small polaron coupling constant, γp, density of states at Fermi level, N(EF) were estimated and discussed.
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25

Abe, Yoshihiro, Hideo Hosono, Osamu Akita, and L. L. Hench. "Protonic Conduction in Phosphate Glasses." Journal of The Electrochemical Society 141, no. 6 (June 1, 1994): L64—L65. http://dx.doi.org/10.1149/1.2054988.

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26

Sharma, Sohan Lal, and D. R. Sharma. "Electrical conduction in Ge1−xPbxSe2 glasses." Physica Status Solidi (a) 127, no. 2 (October 16, 1991): K109—K112. http://dx.doi.org/10.1002/pssa.2211270242.

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27

Usuki, T., K. Nakajima, T. Furukawa, M. Sakurai, S. Kohara, T. Nasu, Y. Amo, and Y. Kameda. "Structure of fast ion conducting AgI–As2Se3 glasses." Journal of Non-Crystalline Solids 353, no. 32-40 (October 2007): 3040–44. http://dx.doi.org/10.1016/j.jnoncrysol.2007.05.036.

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28

Roling, B., and M. D. Ingram. "Mixed alkaline–earth effects in ion conducting glasses." Journal of Non-Crystalline Solids 265, no. 1-2 (March 2000): 113–19. http://dx.doi.org/10.1016/s0022-3093(99)00899-6.

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29

Saha, S. K., and D. Chakravorty. "Inhomogeneous conductor model and fast ion conducting glasses." Journal of Non-Crystalline Solids 167, no. 1-2 (January 1994): 89–91. http://dx.doi.org/10.1016/0022-3093(94)90371-9.

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30

LIN, HONG, FENG HAO, CHUN FU LIN, JIAN BAO LI, and NING WANG. "HIGHLY CATALYTIC ACTIVE NANOSTRUCTURED Pt ELECTRODES FOR DYE-SENSITIZED SOLAR CELLS PREPARED BY LOW TEMPERATURE ELECTRODEPOSITION." Functional Materials Letters 04, no. 01 (March 2011): 7–11. http://dx.doi.org/10.1142/s1793604711001592.

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Highly catalytic active nanostructured Pt electrodes (NPEs) for dye-sensitized solar cells (DSCs) are prepared on indium-doped tin oxide (ITO) conductive glasses using a nonionic surfactant-assisted low-temperature electrodeposition method with controlled quantity of electroplating charge. Transmission electron microscopy (TEM) and scanning electron microscope (SEM) show that the NPEs on ITO conductive glass are composed of nano-sized Pt particles with a diameter of 3–4 nm. Remarkably, with a similar thickness of ca. 38 nm, the NPE shows a charge-transfer resistance (R ct ) of 0.063 Ω ⋅ cm 2, a value almost 20 times lower than that of the sputtered Pt electrode, demonstrating the superior catalytic activity of the NPE. Furthermore, with almost half of the Pt loading, DSC device with NPE exhibits comparable photovoltaic performance with the conventionally sputtered Pt electrode.
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31

Roy, S., and D. Chakravorty. "Electrical conduction in composites of nanosized iron particles and oxide glasses." Journal of Materials Research 9, no. 9 (September 1994): 2314–18. http://dx.doi.org/10.1557/jmr.1994.2314.

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Nanocomposites involving iron particles in silica glass matrix have been synthesized by the hot pressing of suitably reduced precursor gel powders. The metal particles have diameters in the range 3.8 to 10.2 nm. An almost four orders of magnitude resistivity range at room temperature has been obtained by such changes in particle diameters. The resistivity in the temperature range 200-340 K shows a fractional temperature dependence with an average value of n ∼ 0.69. The resistivity changes in this temperature region can be explained on the basis of an electron tunneling mechanism.
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32

Rani, S., S. Sanghi, A. Agarwal, and N. Kishore. "Study of Structure and Li+ Ions Dynamics in Presence of Fe2O3 in Bi2O3∙B2O3 Glasses." Solid State Phenomena 161 (June 2010): 51–61. http://dx.doi.org/10.4028/www.scientific.net/ssp.161.51.

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Glasses having composition xLi2O∙(30-x)Fe2O3∙20Bi2O3∙50B2O3 (0 ≤ x ≤ 30, in mol%) have been prepared using normal melt-quench technique. The variation in density and molar volume with composition has been investigated in terms of the structural modification that takes place in the glass matrix on decreasing Fe2O3. Infrared spectra of these glasses were recorded over continuous spectral range (400-4000 cm-1) in an attempt to study their structure systematically. IR spectra show that with increase in Li2O/Fe2O3 ratio there is formation of more structural units (e.g. [FeO4/2]-Li+) in the glass network. Bi3+ cations are present as [BiO6] octahedral units and acts as modifier in this glass system. Further, the effect of transition metal ions (iron) on the dynamics of lithium bismuth borate glasses has been studied in the frequency range of 20 Hz - 1 MHz and in the temperature range 240 – 350 °C using impedance spectroscopy. Possible conduction mechanisms are discussed. Various AC and DC electrical and dielectric parameters have been calculated and analyzed. The results show that the contribution of electronic conduction towards conductivity decreases with decreasing iron concentration, which is understood to be due to hopping of electrons from Fe2+→Fe3+. The frequency dependent conductivity has been studied using both conductivity and modulus formalism. The absence of maximum observed in dielectric permittivity in the temperature and frequency range studied, indicate the non-ferroelectric behavior of the glasses.
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33

Rossignol, S., B. Tanguy, J. M. Réau, J. J. Videau, and J. Portier. "New Ag+ fast ionic conducting glasses based on Tl4P2O7." Physica Status Solidi (a) 139, no. 2 (October 16, 1993): 337–44. http://dx.doi.org/10.1002/pssa.2211390207.

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34

Wang, Yuhu, Akiyoshi Osaka, and Yoshinari Miura. "Anionic conduction in lead oxyfluoride glasses." Journal of Non-Crystalline Solids 112, no. 1-3 (October 1989): 323–27. http://dx.doi.org/10.1016/0022-3093(89)90546-2.

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35

Skryabin, Y. N. "Relaxation of tunnelling systems by conduction electrons in one dimensional metallic glasses." Solid State Communications 95, no. 3 (July 1995): 195–97. http://dx.doi.org/10.1016/0038-1098(95)00124-7.

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36

Salorkar, Megha A., and V. K. Deshpande. "Study of lithium ion conducting glasses for solid electrolyte application." Physica B: Condensed Matter 627 (February 2022): 413590. http://dx.doi.org/10.1016/j.physb.2021.413590.

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37

Feltz, Adalbert. "Ionic conducting glasses for batteries and wave-guide devices." Journal of Non-Crystalline Solids 90, no. 1-3 (February 1987): 545–55. http://dx.doi.org/10.1016/s0022-3093(87)80483-0.

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38

Deshpande, V. K., Megha A. Salorkar, and Nalini Nagpure. "Study of lithium ion conducting glasses with Li2SO4 addition." Journal of Non-Crystalline Solids 527 (January 2020): 119737. http://dx.doi.org/10.1016/j.jnoncrysol.2019.119737.

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39

Karthikeyan, Annamalai, Chad Martindale, and Steve W. Martin. "Preparation and characterization of new proton conducting chalcogenide glasses." Journal of Non-Crystalline Solids 349 (December 2004): 215–22. http://dx.doi.org/10.1016/j.jnoncrysol.2004.08.145.

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40

Kowada, Y., M. Tatsumisago, T. Minami, and H. Adachi. "Electronic state of sulfide-based lithium ion conducting glasses." Journal of Non-Crystalline Solids 354, no. 2-9 (January 2008): 360–64. http://dx.doi.org/10.1016/j.jnoncrysol.2007.07.085.

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41

Price, David Long, and Adam J. G. Ellison. "Atomic structure and dynamics of fast-ion conducting glasses." Journal of Non-Crystalline Solids 177 (November 1994): 293–98. http://dx.doi.org/10.1016/0022-3093(94)90543-6.

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42

Durand, B., G. Taillades, A. Pradel, M. Ribes, J. C. Badot, and N. Belhadj-Tahar. "Frequency dependence of conductivity in superionic conducting chalcogenide glasses." Journal of Non-Crystalline Solids 172-174 (September 1994): 1306–14. http://dx.doi.org/10.1016/0022-3093(94)90657-2.

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43

Ionescu, Rodica, Raphael Selon, Nicolas Pocholle, Lan Zhou, Anna Rumyantseva, Eric Bourillot, and Eric Lesniewska. "Microwave Spectroscopic Detection of Human Hsp70 Protein on Annealed Gold Nanostructures on ITO Glass Strips." Biosensors 8, no. 4 (November 27, 2018): 118. http://dx.doi.org/10.3390/bios8040118.

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Conductive indium-tin oxide (ITO) and non-conductive glass substrates were successfully modified with embedded gold nanoparticles (AuNPs) formed by controlled thermal annealing at 550 °C for 8 h in a preselected oven. The authors characterized the formation of AuNPs using two microscopic techniques: scanning electron microscopy (SEM) and atomic force microscopy (AFM). The analytical performances of the nanostructured-glasses were compared regarding biosensing of Hsp70, an ATP-driven molecular chaperone. In this work, the human heat-shock protein (Hsp70), was chosen as a model biomarker of body stress disorders for microwave spectroscopic investigations. It was found that microwave screening at 4 GHz allowed for the first time the detection of 12 ng/µL/cm2 of Hsp70.
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44

Dwivedi, S. K., A. Kumar, and S. Kumar. "High-field conduction in some chalcogenide glasses." Advanced Materials for Optics and Electronics 9, no. 6 (November 1999): 235–44. http://dx.doi.org/10.1002/1099-0712(199911/12)9:6<235::aid-amo387>3.0.co;2-q.

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45

Cordes, H., and S. D. Baranovskii. "On the Conduction Mechanism in Ionic Glasses." physica status solidi (b) 218, no. 1 (March 2000): 133–38. http://dx.doi.org/10.1002/(sici)1521-3951(200003)218:1<133::aid-pssb133>3.0.co;2-b.

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46

Kalnaowakun, Phuri, Sutham Niyomwas, and Suchart Chantaramanee. "Comparative Study of Platinum/Single Wall Carbon Nanotube versus Platinum/Carbon Black Coating." Advanced Materials Research 488-489 (March 2012): 928–33. http://dx.doi.org/10.4028/www.scientific.net/amr.488-489.928.

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The study of platinum/carbon black (Pt/CB) versus platinum/single wall carbon nanotubes (Pt/SWCNT) and drying temperature on the result products were investigated. The synthesized of Pt/CB versus Pt/SWCNT were used for coating on fluorine-doped tin oxide (FTO) conductive glasses and tested for electrical conductivity properties used for counter electrode in a dye-sensitized solar cell (DSSC).The result products were characterized in term of chemical composition and microstructure by scanning electron microscope technique (SEM), EDX (JEOL,JSM 5800 LV) and TEM analyses.
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47

Moustafa, Y. M., K. El-Egili, H. Doweidar, and I. Abbas. "Structure and electric conduction of Fe2O3–P2O5 glasses." Physica B: Condensed Matter 353, no. 1-2 (November 2004): 82–91. http://dx.doi.org/10.1016/j.physb.2004.09.004.

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48

Dult, Meenakshi, R. S. Kundu, S. Murugavel, R. Punia, and N. Kishore. "Conduction mechanism in bismuth silicate glasses containing titanium." Physica B: Condensed Matter 452 (November 2014): 102–7. http://dx.doi.org/10.1016/j.physb.2014.07.004.

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49

Herczog, Andrew. "Sodium Ion Conducting Glasses for the Sodium‐Sulfur Battery." Journal of The Electrochemical Society 132, no. 7 (July 1, 1985): 1539–45. http://dx.doi.org/10.1149/1.2114161.

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50

Matusita, Kazumasa, Takayuki Komatsu, and Kazuhiro Aizawa. "An ionic conduction in various fluoride glasses." Journal of Non-Crystalline Solids 95-96 (December 1987): 945–52. http://dx.doi.org/10.1016/s0022-3093(87)80702-0.

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