1983
DOI: 10.1063/1.332180
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Dielectric behavior of red HgI2 under direct bias

Abstract: The dielectric constant and loss were measured at several frequencies and temperatures for red mercuric iodide. The equivalent circuits for the sample, before and after a direct bias has been applied for a long time, are discussed. Complex impedance and loss tangent plots versus frequency and temperature show a contact barrier formation after long time polarization. Results are discussed in terms of gamma radiation detector performance.

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Cited by 20 publications
(5 citation statements)
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“…At low strain rates, the gas bubbles will have a good chance of emerging easily from these cavities and leave the structure, which is highly defected, with low values of yield stress. However, the observed rapid increase of ~y with log E' at low strain rates (or high temperatures) can be understood from the fact that yielding of the composite is dominated by the yield behaviour of steel fibres, which strongly increase with strain rate [17]. At high strain rates, the yielding mechanism is dominated by the yield behaviour of the polymer matrix in the composite, where a linear dependence is observed as in most polymers.…”
Section: Resultsmentioning
confidence: 92%
“…At low strain rates, the gas bubbles will have a good chance of emerging easily from these cavities and leave the structure, which is highly defected, with low values of yield stress. However, the observed rapid increase of ~y with log E' at low strain rates (or high temperatures) can be understood from the fact that yielding of the composite is dominated by the yield behaviour of steel fibres, which strongly increase with strain rate [17]. At high strain rates, the yielding mechanism is dominated by the yield behaviour of the polymer matrix in the composite, where a linear dependence is observed as in most polymers.…”
Section: Resultsmentioning
confidence: 92%
“…The electrical properties of the surface and interfacial layers of dielectric specimens are often different from those of the bulk of the material. These differences are often attributable to contact effects between the electrodes and the specimen [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18]. The phenomenon is important both from the view-point of the measurement and interpretation of the electrical and dielectric properties of dielectrics and from the view-point of the application of these materials in engineering practice.…”
Section: Introductionmentioning
confidence: 99%
“…For thin dielectric and semiconductor specimens, contact effects have a greater influence on the properties of the combination of metallic electrode-dielectric-metallic electrode 0953-8984/97/173609+15$19.50 c 1997 IOP Publishing Ltd than they have for thick specimens, and the difference between measured properties and internal properties becomes correspondingly more significant. These effects have become of practical significance as electrical or microelectronic devices usually incorporate integrated-circuit combinations such as metal-insulator-metal, metal-semiconductor-metal and similar thin-film arrangements [4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19]. In general, these thin-film systems usually involve inhomogeneous parts brought about by structural changes and/or by the creation of surface layers caused by the absorption of atoms, ions or electrons from the surroundings.…”
Section: Introductionmentioning
confidence: 99%
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