|  4-Manifolds | 
Topology > s.a. intersection.
  * Topological classification:
    It is known that a full topological classification is not possible, but one can
    make a list "with repetitions" of all the topologically inequivalent
    manifolds; Some classes can be completely classified.
  $ Homotopy equivalence: Two simply
    connected, compact, oriented 4-manifolds M1
    and M2 are homotopy equivalent iff
    (i) H2(M1;
    \(\mathbb Z\))
    = H2(M2;
    \(\mathbb Z\)), and (ii) Their intersection forms are isomorphic.
  * Result: Two simply connected
    compact 4-manifolds may be homotopic, and possibly homeomorphic, if their Euler
    number χ and Hirzebruch signature τ are equal.
  $ Homeomorphism: Two simply connected,
    compact, oriented 4-manifolds M1 and
    M2 are homeomorphic iff (i) Their
    intersection forms are isomorphic, and (ii) They have the same Kirby-Siebenmann
    invariant; We thus have a classification with 2 invariants.
  * Decidability: 1992, The
    existence of an algorithmic description of the set of compact 4-manifolds
    is an open problem; It depends on the existence of an algorithm
    for recognizing S4.
  * Result: Every connected PL-manifold
    is \(\mathbb R\)4/(some homeomorphism group)
    [@ Lawrence Top(00)].
Differentiable Structures
  * History: 1982, Approach
    to differential topology of 4-manifolds based on gauge theory ideas and
    Yang-Mills instantons introduced; 1994, Seiberg-Witten equation introduced as
    dual approach; Work by Kronheimer, Mrowka, Morgan, Stern, Taubes.
  * Tasks: Identify which
    topological manifolds are realizable as smooth ones, and classify these
    up to diffeomorphisms.
  * Results: \(\mathbb R\) ×
    S3 and \(\mathbb R^4\) admit whole continuous
    families of differentiable structures; Compact 4-manifolds may have countably
    infinite sets of them; For example, CP2
    #9(−P2); Gompf constructed uncountably
    many smoothings of \(\mathbb R\)4 which
    support Stein structures, Taylor showed that uncountably many smoothings of
    \(\mathbb R\)4 support no Stein structure.
  @ Reviews: Iga IJMPA(02)ht [for physicists].
  @ Invariants: Kronheimer & Mrowka JDG(95);
    Fintushel & Stern JDG(97) [and manifold operations];
    Taylor G&T(97) [and Stein structures];
    Pfeiffer PLB(04)gq/03 [and path integral for quantum gravity];
    Fintushel  & Stern Top(04)
      [different, homeomorphic manifolds with same Seiberg-Witten invariants].
  @ Related topics:
    Braungardt & Kotschick Top(05) [and Einstein metrics];
    Akhmedov T&A(04) [constructing exotic ones].
Yang-Mills Instanton (Donaldson) Approach
  * Idea: Based on the
    study of gauge theories (in particular sself-dual connections); A non-standard
    differentiable structure on \(\mathbb R\)4 can
    be obtained from a study of instanton solutions of some gauge theory; In the
    limit when the instanton size goes to zero, the instanton can be associated
    with a point in \(\mathbb R\)4;
    Now, the set of all instanton solutions has a differentiable structure, which
    induces the non-trivial one on \(\mathbb R\)4,
    considered as its boundary.
  @ References:
    Donaldson BAMS(83),
    JDG(83);
    Stern MI(83);
    Fintushel & Stern JDG(84);
    Gompf JDG(85);
    Donaldson Top(90);
    Petrie & Randall 90.
Seiberg-Witten Approach
  * Idea: Based on spinor
    structures and equations with Dirac operators.
  @ Seiberg-Witten equations: Seiberg PLB(93),
    & Witten NPB(94);
    Witten JMP(94),
    MRL(94)ht;
  Donaldson BAMS(96)
  [rev].
  @ Generalizations:
    Acharya et al NPB(97) [higher-dimensional];
    Park NPB(02)ht/01.
Other Structures and Concepts > s.a. 4D
  geometry; Surfaces.
  * Hirzebruch signature: For a compact 4-manifold M,
τ = \(\displaystyle{1\over96\pi^2}\) ∫ Rabcd Rabef εcdef |g|1/2 d4x .
* Examples: τ(S4)
  = 0; τ(\(\mathbb C\)P2)
  = 1; τ(S2-bundle
  over S2) = 0; τ(K3)
  = 16; τ(M1 ×
  M2) = 0 for any two 2D manifolds  M1 and
  M2; Non-compact example, τ(\(\mathbb R\)2)
  = 0.
  @ Subsets: Morgan & Szabó Top(99) [embedded tori].
  @ Related topics: Matveyev dg/95,
  Akbulut & Matveyev IMRN(98)m.GT/00 [decomposition];
  Hegenbarth et al T&A(05)* [connected sums];
    Vajiac IJGMP(10)
      [equivariant localization techniques, and relating Donaldson and Seiberg-Witten invariants].
References
  @ Textbooks and reviews: Lawson 85;
    Freedman & Feng 89;
    Kirby 89;
    Donaldson & Kronheimer 90;
    Freed & Uhlenbeck 90;
    Freedman & Quinn 90;
    Gompf & Stipsicz 99 [and Kirby calculus].
  @ Homeomorphism: Mandelbaum BAMS(80);
    Brown & Thickstun ed-82; Freedman JDG(83);
    van Meter gq/05/CQG [undecidability].
  @ Homotopy equivalence: Whitehead CMH(49).
  @ Cobordisms: Kreck G&T(01).
  @ Invariants: Myers & Periwal NPB(91) [and topological field theory];
    Crane at al ht/93 [Crane-Yetter];
    Crane et al ht/94 [details];
    Mariño & Moore CMP(99) [non-simply connected];
    Marino ht/00-conf [and topological field theory];
    Kronheimer JDG(05)
[from higher-rank bundles];
    McDuff BAMS(06) [and Floer theory, Ozsváth-Szabó].
@ Related topics: Chen et al JDG(12) [classification of compact 4-manifolds with positive isotropic curvature]. 
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