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Breakdown modes, oxide degradation and device drifts under ESD-like stress are discussed as function of the oxide thickness.
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The mechanical and electrical properties of the different composite materials are discussed as functions of the TiN content.
The degree of DNA entrapment, particle morphology, swelling/dissolution behavior and DNA release responses are discussed as functions of the nature of the cationic agent used.
In addition, other critical properties are discussed as functions of the ambient temperature, misfit strain, surface coefficients, work function steps, dielectric constants and screening lengths of electrodes.
In particular, the different aspects of the processing of dielectric layers are discussed as functions of plasma density, pulse duration, and layer characteristics (thickness and permittivity).
The global rates and steady state multiplicities are discussed as functions of particle size, film thickness, gas composition and ambient temperature.
Three important characteristic parameters associated with the sensing application, which are the visibility of the output intensities, the free spectral range and the finesse, are discussed as functions of the coupler coefficients and the fiber loop length in detail.
The procedure B leads to supported RuO2·xH2O particles that appear more crystalline than those obtained by the procedure A. Specific capacitance and specific surface area of the composites are discussed as functions of the RuO2 content, and different dependences for the composites derived from the two carbons are found.
The reinforcement effect in terms of the Young's modulus is discussed as a function of the degree of polymerization of the rods.
The transport rate through the inclusions is also calculated and the degree of utilization of the inclusions is discussed as a function of the volume fractions of inclusions and interphase layer, the size of the inclusions, and the permeability values for the three phases.
Results for the transmission and reflection properties of such circuits are discussed as a function of the wavelength of the excitations and the physical properties of the circuits.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com