By H.-S. Philip Wong, Deji Akinwande
Explaining the houses and function of functional nanotube units and comparable functions, this can be the 1st introductory textbook at the topic. the entire basic innovations are brought, in order that readers with out a sophisticated medical historical past can keep on with all of the significant rules and effects. extra themes lined contain nanotube transistors and interconnects, and the fundamental physics of graphene. challenge units on the finish of each bankruptcy let readers to check their wisdom of the cloth lined and achieve a better realizing of the analytical ability units constructed within the textual content. this can be a great textbook for senior undergraduate and graduate scholars taking classes in semiconductor machine physics and nanoelectronics. it's also an ideal self-study consultant for pro gadget engineers and researchers.
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Extra info for Carbon Nanotube and Graphene Device Physics
This is because the crystal momentum is directly proportional to the wavevector. 7b), the reciprocal lattice is often characterized via X-ray diffraction patterns. First Brillouin zone The ﬁrst Brillouin zone is a central concept in the theory of solids, particularly in the description of the band structure of electrons and other fundamental excitations18 that exist within the solid. We previously discussed the ﬁrst Brillouin zone in the context of the Kronig–Penney model. An equivalent but more basic deﬁnition is available based on the attributes of the reciprocal lattice: the Wigner– Seitz primitive cell of the reciprocal lattice is the ﬁrst Brillouin zone.
Energy and wavevector are actually related, and this relationship is commonly called the dispersion or band structure. It is not an overstatement to assert that the dispersion is the most important and central characteristic that describes the behavior of electrons in a crystalline solid. Indeed, it is the dispersion or band structure that we seek to derive and understand in this chapter, and subsequently in Chapters 3 and 4. It is worthwhile noting that there are a gazillion1 electrons present in typical solids.
Kim, Energy band-gap engineering of graphene nanoribbons. Phys. Rev. , 98 (2007) 206805. 46 Fig. 6. (c) Construct a set of primitive reciprocal lattice vectors for that lattice. (d) Draw the reciprocal lattice. (e) Sketch the ﬁrst Brillouin zone. 7. Bravais and reciprocal lattices. (a) Construct the reciprocal lattice for the ﬁve 2D Bravais lattices. (b) Construct the Brillouin zone for all ﬁve reciprocal lattices. (c) Which of the Bravais lattices yield hexagonal Brillouin zones? 3 Graphene Dream your dreams and may they come true.
Carbon Nanotube and Graphene Device Physics by H.-S. Philip Wong, Deji Akinwande