Page 119 - Science at the nanoscale
P. 119

RPS: PSP0007 - Science-at-Nanoscale
                             8:11
                   June 9, 2009
                             Chapter Six
                             Low-Dimensional Nanostructures
                             In this chapter, we will move from atoms and molecules to the
                             world of solids. Here, we are less concerned with large scale
                             extended solids, where “large scale” here refers to solids with all
                             dimensions larger than about 100 nm, where size-effects do not
                             play a significant role. Instead, we will concern ourselves with
                             “low dimensional” nanostructures, whereby at least one dimen-
                             sion of the solid is less than about 100 nm in length. In such
                             low dimensional systems and nanostructures, the physical prop-
                             erties differ dramatically from those of their corresponding bulk
                             materials because quantum effects become significant. As seen in
                             Chapter 3, confinement of quantum mechanical wave functions in
                             regions of nanoscale dimensions induces a discretisation of energy
                             levels, and in this chapter we will introduce the effects of low
                             dimensionality on the electron density of states and related elec-
                             tronic properties.
                             6.1  FROM 3D TO 0D NANOSTRUCTURES                                     ch06
                             The band theory of solids described in undergraduate solid
                             state physics textbooks is a very successful model for explaining
                             the electronic properties of periodic three-dimensional extended
                             solids. Band theory is based on the assumption that electron prop-
                             erties can be derived by treating the system as a one-electron prob-
                             lem in an average potential determined primarily by the periodic
                             array of ionised atoms in an extended perfect crystal. We will
                             not describe band theory in any detail here, but a useful way
                             Science at the Nanoscale: An Introductory Textbook
                             by Chin Wee Shong, Sow Chorng Haur & Andrew T S Wee
                             Copyright c 
 2010 by Pan Stanford Publishing Pte Ltd
                             www.panstanford.com
                             978-981-4241-03-8
   114   115   116   117   118   119   120   121   122   123   124