By Michael P. Marder(auth.)
This Second Edition offers an up to date overview of the complete box of condensed subject physics. It consolidates new and vintage themes from disparate resources, instructing not just in regards to the powerful plenty of electrons in semiconductor crystals and band thought, but additionally approximately quasicrystals, dynamics of part separation, why rubber is extra floppy than metal, granular fabrics, quantum dots, Berry stages, the quantum corridor influence, and Luttinger liquids.Content:
Chapter 1 the assumption of Crystals (pages 3–16):
Chapter 2 Three?Dimensional Lattices (pages 17–41):
Chapter three Scattering and constructions (pages 43–75):
Chapter four Surfaces and Interfaces (pages 77–95):
Chapter five past Crystals (pages 97–152):
Chapter 6 The unfastened Fermi fuel and unmarried Electron version (pages 155–173):
Chapter 7 Non–Interacting Electrons in a Periodic capability (pages 175–206):
Chapter eight approximately loose and Tightly certain Electrons (pages 207–232):
Chapter nine Electron–Electron Interactions (pages 233–264):
Chapter 10 life like Calculations in Solids (pages 265–292):
Chapter eleven solidarity of Solids (pages 295–319):
Chapter 12 Elasticity (pages 321–329):
Chapter thirteen Phonons (pages 341–378):
Chapter 14 Dislocations and Cracks (pages 379–411):
Chapter 15 Fluid Mechanics (pages 413–449):
Chapter sixteen Dynamics of Bloch Electrons (pages 453–481):
Chapter 17 shipping Phenomena and Fermi Liquid idea (pages 483–521):
Chapter 18 Microscopic Theories of Conduction (pages 523–566):
Chapter 19 Electronics (pages 567–608):
Chapter 20 Phenomenological idea (pages 611–631):
Chapter 21 Optical houses of Semiconductors (pages 633–657):
Chapter 22 Optical homes of Insulators (pages 659–687):
Chapter 23 Optical homes of Metals and Inelastic Scattering (pages 689–720):
Chapter 24 Classical Theories of Magnetism and Ordering (pages 723–758):
Chapter 25 Magnetism of Ions and Electrons (pages 759–795):
Chapter 26 Quantum Mechanics of Interacting Magnetic Moments (pages 797–838):
Chapter 27 Superconductivity (pages 839–894):
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Extra info for Condensed Matter Physics, Second Edition
3. (A) The conventional unit cell of the body-centered cubic lattice (stereo pair). (B) Wigner-Seitz cell of the bcc lattice. The conventional unit cell of the fee lattice is four times as large as a primitive unit cell, as one may determine by considering the fee lattice as a cubic lattice with a basis (Problem 1). More than twenty of the elements adopt the fee lattice, including copper, silver, gold, and the noble gases at low temperatures. 3(A). 3 (B). As in the case of the fee lattice, the lattice constant a refers to the distance between corners of the cube, not to the distance between nearest neighbors.
9. 14. 10, that describe all possible symmetry axes. A dashed line in a stereogram denotes a plane that is not a mirror plane of the object. There are two sets of notation for the crystallographic point groups. 9. In some cases there are two versions of the Schönflies notation, and both are listed. C = Cyclic; allows successive rotation about main axis. D - Dihedral; contains two-fold axes perpendicular to main axis. S = Spiegel; unchanged after combination of reflection and rotation. T = Tetragonal.
Many other historical details are related by Ewald (1962), Phillips (1971), and Hoddeson et al. (1992). This chapter is designed more for reference than for recreational reading. At first the listing of crystal structures may appear more like a dull catalog of animals in some distant land than basic physics. Yet knowledge of crystal structures is the foundation on which much of the rest of condensed matter physics rests. The detailed calculation of electronic and mechanical properties of solids depends on knowing where the atoms lie.