🪡K-Theory Unit 1 – Introduction to Vector Bundles and K–Theory
K-Theory provides a powerful framework for studying vector bundles, combining ideas from algebraic topology, differential geometry, and abstract algebra. It allows for the classification of vector bundles using K-groups, abelian groups associated with topological spaces, and enables the computation of important invariants.
This unit introduces key concepts like vector bundles, sections, trivial bundles, and isomorphisms. It explores the historical development of K-Theory, from Grothendieck's work in the 1950s to its applications in diverse areas like operator algebras, mathematical physics, and algebraic geometry.
K-Theory provides a powerful framework for studying vector bundles and their properties
Combines ideas from algebraic topology, differential geometry, and abstract algebra to gain deeper insights into the structure of vector bundles
Allows for the classification of vector bundles up to isomorphism using K-groups, which are abelian groups associated with a topological space
Enables the computation of important invariants (characteristic classes) that capture essential information about the geometry and topology of vector bundles
Provides a unified language for understanding and comparing vector bundles across different contexts (smooth manifolds, algebraic varieties, etc.)
Facilitates the transfer of ideas and techniques between these different settings
Connects to other areas of mathematics, such as index theory and operator algebras, leading to fruitful interactions and applications
Serves as a bridge between classical algebraic topology and modern developments in geometry and physics (gauge theory, string theory)
Key Concepts and Definitions
Vector bundle: a family of vector spaces parametrized by a topological space, with a locally trivial structure
Consists of a total space E, a base space B, and a projection map π:E→B
Each fiber π−1(b) is a vector space isomorphic to a fixed model space (typically Rn or Cn)
Sections of a vector bundle: continuous maps s:B→E such that π∘s=idB, assigning a vector to each point in the base space
Trivial bundle: a vector bundle isomorphic to the product bundle B×Rn (or B×Cn)
Isomorphism of vector bundles: a fiber-preserving homeomorphism between the total spaces that restricts to linear isomorphisms on each fiber
K-group: an abelian group associated with a topological space X, denoted K(X), whose elements represent stable isomorphism classes of vector bundles over X
The group operation is induced by the direct sum of vector bundles
Reduced K-theory: a variant of K-theory that assigns the trivial group to a point, denoted K~(X)
Characteristic classes: cohomology classes associated with vector bundles that capture geometric and topological properties (Chern classes, Pontryagin classes, Euler class)
Historical Context and Development
Origins in the work of Alexander Grothendieck in the 1950s, who introduced K-theory for algebraic varieties as a tool for studying coherent sheaves
Michael Atiyah and Friedrich Hirzebruch developed topological K-theory in the 1960s, extending Grothendieck's ideas to the context of topological spaces and vector bundles
Their seminal paper "Vector bundles and homogeneous spaces" (1961) laid the foundations for the subject
Atiyah and Isadore Singer's work on the index theorem (1963) revealed deep connections between K-theory, differential geometry, and elliptic differential operators
The Atiyah-Hirzebruch spectral sequence, introduced in their 1961 paper, provided a powerful computational tool for calculating K-groups
Further developments by Raoul Bott, Graeme Segal, and others in the 1960s and 1970s expanded the scope and applications of K-theory
Bott periodicity, the Thom isomorphism, and the Segal conjecture are notable examples
In the 1980s and beyond, K-theory found applications in diverse areas such as operator algebras (C*-algebras, von Neumann algebras), mathematical physics (gauge theory, string theory), and algebraic geometry (motivic cohomology)
Vector Bundles: The Basics
A vector bundle π:E→B consists of a total space E, a base space B, and a projection map π satisfying certain local triviality conditions
For each point b∈B, there exists a neighborhood U and a homeomorphism ϕ:π−1(U)→U×Rn (or U×Cn) such that π=pr1∘ϕ
The rank of a vector bundle is the dimension of its fibers (the vector spaces π−1(b))
Examples of vector bundles include the tangent bundle and normal bundle of a smooth manifold, the tautological line bundle over projective space, and the Möbius band
Operations on vector bundles:
Direct sum: given bundles E1 and E2 over B, their direct sum E1⊕E2 is a new bundle with fibers (E1⊕E2)b=(E1)b⊕(E2)b
Tensor product: the tensor product E1⊗E2 has fibers (E1⊗E2)b=(E1)b⊗(E2)b
Dual bundle: the dual bundle E∗ has fibers (E∗)b=((E)b)∗, the dual vector space
The Whitney sum formula relates the characteristic classes of a direct sum to those of its summands
The pullback construction allows for the transfer of vector bundles along continuous maps between topological spaces
K-Theory: A New Perspective
K-theory associates an abelian group K(X) to each topological space X, whose elements represent stable isomorphism classes of vector bundles over X
Two vector bundles E1 and E2 are stably isomorphic if there exist trivial bundles ε1 and ε2 such that E1⊕ε1≅E2⊕ε2
The group operation in K(X) is induced by the direct sum of vector bundles, with the trivial bundle serving as the identity element
Reduced K-theory K~(X) is defined as the kernel of the map K(X)→K(point) induced by the constant map X→point
Fits into a split short exact sequence 0→K~(X)→K(X)→Z→0, with the rank function providing a splitting
K-theory is a generalized cohomology theory, satisfying the Eilenberg-Steenrod axioms (except the dimension axiom)
Functorial with respect to continuous maps, with induced homomorphisms f∗:K(Y)→K(X) for f:X→Y
Satisfies the homotopy invariance and Mayer-Vietoris sequence axioms
The Bott periodicity theorem states that K(X)≅K(Σ2X), where Σ2X is the double suspension of X
Implies that the K-groups of a space exhibit a periodic pattern, with K−n(X)≅K−n−2(X)
The Thom isomorphism theorem relates the K-theory of a vector bundle to that of its base space, providing a powerful computational tool
Important Theorems and Proofs
The Atiyah-Hirzebruch spectral sequence relates the K-theory of a space to its ordinary cohomology, providing a means for computing K-groups
The E2 page of the spectral sequence is given by E2p,q=Hp(X;Kq(point)), with differentials dr:Erp,q→Erp+r,q−r+1
Converges to the associated graded of a filtration on K(X)
The Thom isomorphism theorem states that for a rank n vector bundle π:E→B, there is an isomorphism ϕ:K(B)→K~(E), called the Thom class
The Thom class is natural with respect to pullbacks and satisfies a multiplicative property with respect to the tensor product of bundles
The Chern character is a ring homomorphism ch:K(X)→H∗(X;Q) that relates K-theory to rational cohomology
Defined in terms of the Chern classes of a vector bundle, with ch(E)=∑i=0∞i!1ci(E)
Becomes an isomorphism after tensoring with the rational numbers
The Adams operations ψk:K(X)→K(X) are ring homomorphisms that provide a way to study the structure of K-theory
Defined in terms of the exterior powers of a vector bundle, with ψk(E)=∑i=0rank(E)(−1)i(ik)Λi(E)
Satisfy the identity ψk∘ψl=ψkl and are related to the Chern character by ch∘ψk=k∗∘ch, where k∗ is the map induced by the multiplication by k on rational cohomology
The Segal conjecture, proved by Graeme Segal in the 1970s, provides a description of the K-theory of the classifying space BG of a compact Lie group G in terms of the representation ring R(G)
Real-World Applications
K-theory has found applications in various branches of physics, particularly in the study of topological phases of matter and the classification of topological insulators and superconductors
The K-theory of the Brillouin zone (a torus in momentum space) captures the topological properties of electronic band structures
The bulk-boundary correspondence relates the K-theory of the bulk material to the existence of topologically protected edge states
In string theory, K-theory provides a framework for understanding D-brane charges and the classification of Ramond-Ramond fields
The K-theory of spacetime is used to define the charge groups of D-branes, with stable isomorphism classes of vector bundles corresponding to different brane configurations
K-theory has also been applied to the study of symmetry-protected topological phases and the classification of crystalline solids
The K-theory of the space of symmetry-preserving Hamiltonians captures the topological invariants that distinguish different phases
In algebraic geometry, K-theory is used to study the category of coherent sheaves on a scheme or algebraic variety
The Grothendieck group of the category of coherent sheaves, denoted K0(X), provides a useful invariant for studying the geometry of the variety
Higher K-groups, such as K1(X) and K2(X), capture more refined information about the category of vector bundles and their automorphisms
K-theory has also found applications in operator algebras and noncommutative geometry, where it is used to study the structure of C*-algebras and their modules
The K-theory of a C*-algebra A, denoted K0(A) and K1(A), provides a powerful invariant for distinguishing nonisomorphic algebras and understanding their properties
Common Pitfalls and How to Avoid Them
Confusing stable isomorphism with isomorphism: remember that K-theory captures information up to stable equivalence, which allows for the addition of trivial bundles
To avoid this, always consider bundles up to stable isomorphism and be mindful of the role of trivial bundles in the equivalence relation
Neglecting the role of the base space: the K-theory of a space depends crucially on the topology of the base, not just the fibers
Always consider the full data of a vector bundle, including the base space and the projection map, rather than just focusing on the fibers
Misapplying the Bott periodicity theorem: the periodicity applies to the K-groups of a space, not to the space itself
Be careful when using Bott periodicity to compute K-groups, and make sure to apply the theorem correctly to the K-groups rather than the underlying topological space
Overlooking the role of compact support: when working with non-compact spaces, it is often necessary to consider vector bundles with compact support or to use compactly supported K-theory
Be mindful of the support of the bundles you are working with, and use the appropriate version of K-theory for the situation at hand
Mishandling the signs and gradings in the Mayer-Vietoris sequence: the connecting homomorphism in the Mayer-Vietoris sequence involves a sign that depends on the degree of the K-group
Pay close attention to the signs and gradings when using the Mayer-Vietoris sequence to compute K-groups, and be consistent in your choice of conventions
Forgetting the hypotheses of theorems: many important results in K-theory, such as the Thom isomorphism and the Chern character, have specific hypotheses that must be satisfied for the theorems to hold
Always check that the hypotheses of a theorem are satisfied before applying it, and be aware of any limitations or restrictions on its use
Confusing the different versions of K-theory: there are many variants of K-theory, such as topological, algebraic, and operator K-theory, each with its own specific definitions and properties
Be clear about which version of K-theory you are using, and make sure to use the appropriate definitions and results for that particular variant
Not exploiting the full power of the tools: K-theory provides a rich toolkit for studying vector bundles and their properties, but it can be easy to overlook some of the more advanced techniques
Take the time to learn about the various tools and techniques available in K-theory, such as the Atiyah-Hirzebruch spectral sequence, the Adams operations, and the Chern character, and use them to their full potential in your work