By Vladimir V. Mitin, Viatcheslav A. Kochelap, Michael A. Stroscio
This textbook is a complete, interdisciplinary account of the expertise and technology underpinning nanoelectronics, overlaying the underlying physics, nanostructures, nanomaterials, and nanodevices. It offers a unifying framework for the fundamental rules had to comprehend the advancements within the box. After introducing the hot developments in semiconductor and machine nanotechnologies, in addition to novel machine ideas, the tools of progress, fabrication and characterization of fabrics for nanoelectronics are mentioned. insurance then strikes to an research of nanostructures together with recently-discovered nanoobjects, and concludes with a dialogue of units that use a 'simple' scaling-down method of replica recognized microelectronic units, and nanodevices in line with new rules that can not be learned on the macroscale. With various illustrations and homework difficulties, this textbook is appropriate for complex undergraduate and graduate scholars in electric and digital engineering, nanoscience, fabrics, bioengineering and chemical engineering. Addtional assets, together with instructor-only options and Java applets, can be found from www.cambridge.org/9780521881722.
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Additional resources for Introduction to Nanoelectronics: Science, Nanotechnology, Engineering, and Applications
By analyzing particle motion, we have seen that at small spatial scales a particle can not be characterized by exact coordinates and momentum (velocity) and behaves rather as an extended wave-like object. Thus, wave properties and particle properties for the same physical object are compatible. This is the essence of wave–particle duality; indeed, this is an underlying principle of central importance for nanophysics. Contemporary microelectronics and optoelectronics exploit electric and light phenomena, which are determined entirely by the properties of electrons in solids.
4) where ψ(r) is a complex function of the spatial coordinates only. The time-dependent wavefunction, (r, t), is often called the non-stationary wavefunction, while ψ(r) is referred to as a stationary wavefunction. By substituting Eq. 4) into Eq. 1), one gets the time-independent Schr¨odinger equation: − -h2 ∇ 2 + V (r) ψ(r) = Eψ(r). 5) In Eqs. 5), E is the total energy of a particle. One of the important properties of solutions to Eq. 6) where δi j = 1, 0, if i = j, if i = j. The major task of quantum mechanics is to solve the Schr¨odinger wave equation, Eq.
Estimate the density of quanta Nq,b . 1 Introduction In this chapter we discuss the basic physical concepts and equations related to the behavior of particles in the nanoworld. We introduce the Schr¨odinger wave equation for particles and determine the ways to calculate observable physical quantities. , such a motion is quantized. , free motion) is not quantized and is described by propagating waves, the energy of the particle is characterized by a continuous range of values. Keeping in mind the diverse variants of nanostructures, by using wave mechanics we analyze some particular examples, which highlight important quantum properties of particles.