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Rev. Math. Phys. 6, 319–342 (1994) 24. : Cohomology groups for projection tilings of codimension 2. Mat. Sci. Eng. A 294–296, 438–440 (2000) 25. : Algebraic topology for minimal Cantor sets. uchile. pdf 26. : Topological Dynamics. providence RI: Amer. Math. , 1955 27. : Principles of Algebraic Geometry. New York: Wiley 1978 28. , Gratias, D. : Lectures on Quasicrystals. Les Ulis: Editions de Physique, 1994 29. : The rotation number for almost periodic potentials. Commun. Math. Phys. 84 403–438 (1982) 30.
4 Local uniformizers . . . . . . . . . . 3. Virtual Moduli Cycles . . . . . . . . . . . . . 1 The local construction . . . . . . . . . . . . 2 The global construction . . . . . . . . . . . The author was supported in part by NNSF 19971045 and 10371007 of China. . 44 . . . 49 49 . . . . . 51 52 55 55 56 58 59 59 59 64 . . . . . . . . . . 44 4. Gromov-Witten Invariants . . . . . . . . . . . . 1 Definition and simple properties .
Namely any ∗ -isomorphism α : A → B between C ∗ -algebrasinduces a group homomorphism α∗ defined by α∗ ([P ]) = [α(P )] for K0 and similarly for K1 . Moreover, K(lim An ) = lim K(An ). → → For the purpose of this paper some more details will be needed in connection with the Bott periodicity. More precisely, a ∗-algebra A is called a local Banach algebra (LB) if it is normed and if it is invariant by holomorphic functional calculus. Then K(A) can be defined in a way similar to the case of C ∗ -algebras.