Book contents
- Frontmatter
- Contents
- Introduction
- 1 Revision of basic structures
- 2 Duality between geometry and algebra
- 3 The quantum general linear group
- 4 Modules and tensor products
- 5 Cauchy modules
- 6 Algebras
- 7 Coalgebras and bialgebras
- 8 Dual coalgebras of algebras
- 9 Hopf algebras
- 10 Representations of quantum groups
- 11 Tensor categories
- 12 Internal homs and duals
- 13 Tensor functors and Yang–Baxter operators
- 14 A tortile Yang–Baxter operator for each finite–dimensional vector space
- 15 Monoids in tensor categories
- 16 Tannaka duality
- 17 Adjoining an antipode to a bialgebra
- 18 The quantum general linear group again
- 19 Solutions to Exercises
- References
- Index
2 - Duality between geometry and algebra
Published online by Cambridge University Press: 15 December 2009
- Frontmatter
- Contents
- Introduction
- 1 Revision of basic structures
- 2 Duality between geometry and algebra
- 3 The quantum general linear group
- 4 Modules and tensor products
- 5 Cauchy modules
- 6 Algebras
- 7 Coalgebras and bialgebras
- 8 Dual coalgebras of algebras
- 9 Hopf algebras
- 10 Representations of quantum groups
- 11 Tensor categories
- 12 Internal homs and duals
- 13 Tensor functors and Yang–Baxter operators
- 14 A tortile Yang–Baxter operator for each finite–dimensional vector space
- 15 Monoids in tensor categories
- 16 Tannaka duality
- 17 Adjoining an antipode to a bialgebra
- 18 The quantum general linear group again
- 19 Solutions to Exercises
- References
- Index
Summary
The purpose of this section is to convince you that commutative algebras are really spaces seen from the other side of your brain.
For a compact hausdorff space X, we have the algebra C(X) of continuous, complex-valued functions a : X → ℂ. The addition and multiplication are obtained pointwise from ℂ.
A continuous function ƒ : X → Y gives rise to an algebra morphism C(ƒ) : C(Y) → C(X) (note the reversal of direction!) via C(ƒ)(b) = a, where a (x) = b(ƒ(x)). In particular, the unique X → 1 gives the algebra morphism η : ℂ = C(1) → C(X), while each point x : 1 → X of the space gives an algebra morphism C(X) → ℂ.
Actually C(X) is more than just a ℂ-algebra; it is what is called a commutative C*-algebra (there is a norm and an involution (_)* coming from conjugation). With this extra structure the duality becomes precise:
Each commutative C*-algebra A is isomorphic to C(X) for some compact hausdorff space X; each C*-algebra morphism C(Y) → C(X) has the form C(ƒ) for a unique continuous function ƒ : X → Y.
This result is commonly referred to as Gelfand duality.
Algebraic geometry is the study of spaces called varieties: the solutions to polynomial equations in several variables. In studying the variety given by x2 + 2y3 = z4 over the field k, we pass to the k-algebra
By k[x, y, z] we mean the k-algebra of polynomials in three commuting indeterminates x, y, z; the elements are expressions
where αijk ∈ k and (i, j,k) runs over a finite subset of ℕ3.
- Type
- Chapter
- Information
- Quantum GroupsA Path to Current Algebra, pp. 5 - 8Publisher: Cambridge University PressPrint publication year: 2007