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Frequency and voltage dependence of dielectric properties, complex electric modulus, and electrical conductivity in Au/7% graphene doped‐PVA/n‐Si (MPS) structures
Author(s) -
Altındal Yerişkin Seçkin,
Balbaşı Muzaffer,
Tataroğlu Adem
Publication year - 2016
Publication title -
journal of applied polymer science
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.575
H-Index - 166
eISSN - 1097-4628
pISSN - 0021-8995
DOI - 10.1002/app.43827
Subject(s) - materials science , dielectric , dissipation factor , permittivity , capacitance , conductivity , electrical resistivity and conductivity , relaxation (psychology) , condensed matter physics , doping , electrical engineering , chemistry , physics , electrode , optoelectronics , engineering , psychology , social psychology
ABSTRACT In order to increase the capacitance of Au/n‐Si (MS) structure, 7% graphene doped PVA was coated on n‐Si as an interfacial layer. The measured data of capacitance ( C ) and conductance ( G /ω) of Au/7% graphene doped‐PVA/n‐Si (MPS) structure was utilized for the calculation of real and imaginary parts of complex permittivity (ε * = ε′ − j ε″), loss tangent (tanδ), complex electric modulus ( M * = M ′ + jM″ ), and electrical conductivity (σ). The admittance measurements ( C and G /ω) were carried out in the frequency range of 0.5 kHz to 1 MHz at room temperature. Frequency dependence of the dielectric constant (ε′), dielectric loss (ε″) and tanδ shows a dispersive behavior at low frequencies. This behavior was explained by Maxwell–Wagner relaxation. Due to the dipolar and the interfacial polarizations, as well as the surface states ( N ss ) and the interfacial PVA layer, the parameters exhibited a strong dependence on frequency and applied bias voltage. The σ versus log( f ) plot exhibited both low and high frequency dispersion phenomena such that at low frequencies σ value corresponding to the dc conductivity (σ dc ), but at high frequencies it corresponds to the ac conductivity (σ ac ). M ′ and M ″, both, have low values in the low frequency region. However, an increase is observed with the increasing frequency due to the short‐range mobility of charge carriers. As a result, the change in dielectric parameters and electric modulus with frequency is the result of relaxation phenomena and surface states. © 2016 Wiley Periodicals, Inc. J. Appl. Polym. Sci. 2016 , 133 , 43827.