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Reports have shown that a high degree of oxygen defects were introduced in the hole-conducting MoO3 layer by annealing the devices under vacuum (~10−5 mbar) at nominal temperature (120 °C) and time (10 min).
Subsequently, random point defects were introduced in the ordered pattern in order to study the influence of disorder on the reflection spectra and to establish the presence of localized modes.
It was indicated that formation of the defects and structural modifications take place in muscovite mica as a result of swift heavy ion irradiation, and it was found that more defects were introduced in mica by irradiation with higher ion fluences and higher electronic stopping power Se values.
It is found that at room temperature, defects were introduced in MWCNTs under 70 keV N+ ion beam irradiation at a low dose of 1 × 1016 ions/cm2 while MWCNTs transformed into a-CNWs at a high dose of 7 × 1016 ions/cm2.
Mann et al. [5] reported that the bonding strength between human femur and cement depended on the amount of bone interdigitated with PMMA cement, with a mean fracture energy measured as 350 J/m for mode I and 1000 J/m for mode II, although no defects were introduced in these tests.
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The most notable differences are observed when defects are introduced in the metal/semiconductor junctions.
The vacancy-type defects are introduced in the first interfacial TiO2 layer.
Vacancy defects are introduced in the scattering region, while no defects are present in the left and right leads.
In this study, solvent-like defects are introduced in the center of the PEO chain to reduce its crystallinity with the aim to enhance ion conductivity.
The local defect is introduced in the form of missing strut for the unit cell.
Even when a defect is introduced in the computed problems, different numerical solutions are found.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com