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In the chapter, devoted to the theory of $C^*$-algebras, we pay special attention to graded and real $C^*$-algebras. An important role in the sequel is play by the $C^*$-modules and invariant traces. The theory of $C^*$-algebras is closely related to the theory of $C^*$-dynamic systems and crossed products. We also briefly recall basics of the theory of von Neumann algebras and $W^*$-dynamic systems. The $K$-theory is a natural mathematical language for the description of solid state physics. In the chapter, devoted to this theory, we consider in detail the topological $K$-groups amd algebraic ones as well. The topological invariants of solid bodies are defined on the base of the index theory of $\mathcal T$-Fredholm operators. The main invariants are given by the Chern cocecles defined in terls of cyclic cohomologies. The developed mathematical methods are applied to the theory of solid states. Of special interest is the so called BB-correspondence connecting the topological invariants of the solid body with topological invariants of its boundary. An important role in the solid state physics is played by graphene. This is a solid body with sexagonal crystal lattice having carbon atoms in its sites. Graphene and uts topological properties are considered in the kast chapter of the course. PROGRAM
II. BLOCH THEORY
2.2. Physical interpretation 2.3. Fermion Fock space 2.4. Fermion Fock space of the solid body
3.2. Graded and real $C^*$-algebras 3.3. Clifford algebras 3.4. $C^*$-modules 3.5. $C^*$-dynamical systems and crossed products 3.6. $W^*$-dynamical systems 3.7. Invariant traces
4.2. Grothendieck construction 4.3. Algebraic $K_0$-group 4.4. $K_1$-group 4.5. Algebraic $K_1$-group 4.6. Higher $K$-groups
5.2. $\mathcal T$-Fredholm operators 5.3 Cyclic cohomologies 5.4. Chern cocycles and Toeplitz operators 5.5. Toeplitz extensions
6.2. Halfspace and boundary algebras 6.3. Topological invariants of the solid state 6.4. Smooth $BB$-correspondence
7.2. Topological invariants of graphene RSS: Forthcoming seminars
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