Page 95 - Semiconductor For Micro- and Nanotechnology An Introduction For Engineers

The Crystal Lattice System
cal phonons explain why a solid lattice is able to interact with light. With
the simpler harmonic model we already obtain useful expressions for the
heat capacity and thermal expansion. In Chapter 7 we will see that for a
realistic model of the heat conductivity, this model must be extended.

2.7 References for Chapter 2

2.1 Neil W. Ashcroft, N. David Mermin, Solid State Physics, Saunders
College Publishing, Philadelphia (1988)
2.2 H. Lüth, Surfaces and Interfaces of Solid Materials, 3rd Ed.,
Springer Verlag, Berlin (1995)
2.3 Marie-Catharin Desjonquères, D. Spanjaard, Concepts in Surface
Physics, 2nd Ed., Springer Verlag, Berlin (1996)
2.4 Otfried Madelung, Introduction to Solid-State Theory, Springer-
Verlag, Heidelberg (1981)
2.5 Otfried Madelung, Semiconductors - Basic Data, Springer-Verlag,
Heidelberg (1996)
2.6 Arokia Nathan, Henry Baltes, Microtransducer CAD, Springer-
Verlag, Vienna (1999)
2.7 D. F. Nelson, Electric, Optic and Acoustic Interactions in Dielec-
trics, John Wiley and Sons, New York (1979)
2.8 Frank H. Stillinger, Thomas A. Weber, Computer Simulation of
Local Order in Condensed Phases of Silicon, Phys. Rev. B, 31(8)
(1985) pp. 5262–5271
2.9 Simon M. Sze, Physics of Semiconductor Devices, 2nd Ed., John
Wiley and Sons, New York (1981)
2.10 Franklin F. Y. Wang, Introduction to Solid State Electronics, 2nd
Ed., North-Holland, Amsterdam (1989)
2.11 Abraham I. Beltzer, Acoustics of Solids, Springer Verlag, Berlin
(1988)
2.12 R. W. H. Stevenson, ed., Phonons in Perfect Lattices and in Lattices
with Point Defects, Scottish Universities Summer School 1965,
Oliver & Boyd, Edinburgh (1966). Chapter 1, General Introduc-
tion, by C. Kittel, Chapter 2, Phonons in Perfect Lattices, by W.
Cochran.

92 Semiconductors for Micro and Nanosystem Technology