INTRODUCTION
7
developed before they will have an impact on technology. Michael Roukes, who is
working on development of nanoelectromechanical devices, has pointed out some
other challenges in the September 2001 issue of Scient& American. One major
challenge deals with communication between the nanoworld and the macroworld.
For example, the resonant vibrational frequency of a rigid beam increases as the size
of the beam decreases. In the nanoregime the frequencies can be as high 10" Hertz,
and the amplitudes of vibration in the picometer (10-l2) to femtometer
range. The sensor must be able to detect these small displacements and high
frequencies. Optical deflection schemes, such as those used in scanning tunneling
microscopy discussed in Chapter 3, may not work because of the diffraction limit,
which becomes a problem when the wavelength of the light is in the order of the size
of the object from which the light is to be reflected. Another obstacle to be overcome
is the effect of surface on nanostructures. A silicon beam lOnm wide and l o o m
long has almost 10% of its atoms at or near the surface. The surface atoms will affect
the mechanical behavior (strength, flexibility, etc.) of the beam, albeit in a way that is
not yet understood.
7
developed before they will have an impact on technology. Michael Roukes, who is
working on development of nanoelectromechanical devices, has pointed out some
other challenges in the September 2001 issue of Scient& American. One major
challenge deals with communication between the nanoworld and the macroworld.
For example, the resonant vibrational frequency of a rigid beam increases as the size
of the beam decreases. In the nanoregime the frequencies can be as high 10" Hertz,
and the amplitudes of vibration in the picometer (10-l2) to femtometer
range. The sensor must be able to detect these small displacements and high
frequencies. Optical deflection schemes, such as those used in scanning tunneling
microscopy discussed in Chapter 3, may not work because of the diffraction limit,
which becomes a problem when the wavelength of the light is in the order of the size
of the object from which the light is to be reflected. Another obstacle to be overcome
is the effect of surface on nanostructures. A silicon beam lOnm wide and l o o m
long has almost 10% of its atoms at or near the surface. The surface atoms will affect
the mechanical behavior (strength, flexibility, etc.) of the beam, albeit in a way that is
not yet understood.