Impedance analysis of TeO2-SeO2-Li2O nano glass system

被引:22
作者
Rao, P. Satya Gopal [1 ]
Siripuram, Rajesh [2 ]
Sripada, Suresh [2 ]
机构
[1] AlHabeeb Coll Engn & Tech, Dept Phys, Chevella, Telangana, India
[2] JNTUHCEJ, Dept Phys, Karimnagar, Telangana, India
关键词
Nano crystallization; Nano glasses; Nanorods; Impedance analysis; AC and DC conductivity; ELECTRICAL-PROPERTIES; AC CONDUCTIVITY; SPECTROSCOPY; LITHIUM; NANOCRYSTALLIZATION; FABRICATION; RELAXATION; BEHAVIOR; KINETICS; SPECTRA;
D O I
10.1016/j.rinp.2019.02.069
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Nano crystallization in tellurium selenite glasses (TeO2-SeO2-Li2O) is achieved by the conventional heat treatment method. The structural phase transformation of glass samples is verified by X-Ray diffraction. The morphology, crystallinity, and the size of crystals were determined by Field Emission Scanning Electron Microscopy. The main crystalline phases detected are Li2Te2O5 vertical bar alpha-Li2Te2O5, TeO2, Li2TeO3, SeO2, Li2Te2O5 vertical bar beta-Li2Te2O5, Se. It is found that nanoparticles are agglomerated into a rod-like structure having size in the range of 20-93 nm. Conduction mechanism and relaxation behavior in the present glass system is studied with a function of temperature and frequency. The conductivity is slightly increased from 1.04x10(-4) to 2.87 x 10(-4) Omega(-1) m(-1) as the temperature is increased from 100 to 250 degrees C. It is observed that the electrical resistance decreases as the Li2O concentration is increased from 10 to 20 mol %. From the modulus spectra, the presence of both grain and grain boundary effect is observed. From the data, the hump is observed around temperature 200 degrees C in the tested glass system and indicates transition which represents resonance in the glass system due to nano crystalline behavior in the glass matrix. The power law exponent is calculated by fitting the data and suggesting those ideal long-range pathways, diffusion-limited hopping in the glass sample. Based on exponent values, ionic conductivity exists in the glass sample.
引用
收藏
页数:13
相关论文
共 39 条
[1]   Nanocrystalline patterning of K3Li2Nb5O15 on TeO2 glasses by an excimer laser [J].
Ahamad, M. Niyaz ;
Mizuno, Shintaro ;
Komatsu, Takayuki ;
Varma, K. B. R. .
JOURNAL OF CRYSTAL GROWTH, 2007, 304 (01) :270-274
[2]  
Ahmed MA., 2012, World Journal of Condensed Matter Physics, V2, P66, DOI [10.4236/wjcmp.2012.22012, DOI 10.4236/WJCMP.2012.22012]
[3]   Nanocrystallization as a method of improvement of electrical properties of Fe2O3-PbO2-TeO2 glasses [J].
Al-Assiri, M. S. ;
El-Desoky, M. M. .
JOURNAL OF MATERIALS SCIENCE-MATERIALS IN ELECTRONICS, 2014, 25 (09) :3703-3711
[4]   Impedance spectroscopy of V2O5-Bi2O3-BaTiO3 glass-ceramics [J].
Al-syadi, Aref M. ;
Yousef, El Sayed ;
El-Desoky, M. M. ;
Al-Assiri, M. S. .
SOLID STATE SCIENCES, 2013, 26 :72-82
[5]   Dielectric and AC conductivity studies in Li2O-CoO-B2O3-TeO2 glasses [J].
Ashwajeet, J. S. ;
Sankarappa, T. .
IONICS, 2017, 23 (03) :627-636
[6]   Structure and properties of a non-traditional glass containing TeO2, SeO2 and MoO3 [J].
Bachvarova-Nedelcheva, A. ;
Iordanova, R. ;
Kostov, K. L. ;
Yordanov, St ;
Canev, V. .
OPTICAL MATERIALS, 2012, 34 (11) :1781-1787
[7]   MIXED-ALKALI EFFECT IN THE 30[(1-X)LI2O-CENTER-DOT-XNA(2)O]70TEO2 GLASS SYSTEM [J].
BALAYA, P ;
SUNANDANA, CS .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 1994, 175 (01) :51-58
[8]  
Barik S.K., 2011, ADV MAT LETT, V2, P419, DOI [DOI 10.5185/amlett.2011.2228, DOI 10.5185/AMLETT.2011.2228, 10.5185/amlett.2011.2228]
[9]   Interpretation of dc and ac conductivity of Ag2O-SeO2-MoO3 glass-nanocomposite-semiconductor [J].
Bhattacharya, Sanjib ;
Kundu, Ranadip ;
Das, Anindya Sundar ;
Roy, Debasish .
MATERIALS SCIENCE AND ENGINEERING B-ADVANCED FUNCTIONAL SOLID-STATE MATERIALS, 2015, 197 :51-57
[10]   RELAXATION AND FLUCTUATIONS IN GLASSY FAST-ION CONDUCTORS - WIDE-FREQUENCY-RANGE NMR AND CONDUCTIVITY MEASUREMENTS [J].
BORSA, F ;
TORGESON, DR ;
MARTIN, SW ;
PATEL, HK .
PHYSICAL REVIEW B, 1992, 46 (02) :795-800