|  Fixed-Point Theorems | 
In General > s.a. posets.
  * Simple example:
    If I hold a map of an area including the point where I stand, there must
    be a point on the map which is exactly above the corresponding point
    of the real world (even if I deform or crumple the map).
  * Motivation: If A
    is any differential operator, the existence of solutions of the equation
    A f = 0 is equivalent to the existence of fixed points for
    A + I; We are interested in equations like df = 0 for
    the study of critical points (> see morse
    theory, etc).
  * Applications: The
    earliest one was to the existence of periodic orbits for 3 bodies.
  @ General references: Granas & Dugundji
      03;
    Farmakis & Moskowitz 13 [and applications].
  @ Various types: Prykarpatsky a0902 [Leray-Schauder, Borsuk-Ulam type generalization].
  > Online resources:
    see Wikipedia page.
Simple Case: Real Functions of One Variable
  $ Def: Given any interval
    [a, b] ⊂ \(\mathbb R\), any f : [a,
    b] → [a, b] must have at least one fixed point
    (the graph must cross at least once the line x = y).
Brouwer Fixed-Point Theorem
  $ Def: Any continuous f :
    Dn → Dn
    has (at least) one fixed point (Dn is the
    n-dimensional ball).
  * Special cases: For n = 2, it
    can be proved using the fundamental group, through the fact that S1 is
    not a retract of D2 (in general, it is done using
    higher-order homotopy groups, or considering the index of the vector field
    v(x):= x − f(x),
    at different points with respect to different loops).
Lefschetz Fixed-Point Theorem
  * Idea: Let S be
    an n-dimensional manifold (or "almost"), and f
    a map f : S → S; Then f induces a
    map f* of the homology groups,
f*: Hi → Hi, for i = 1, ..., n,
and from these we can define some numbers ni, which are something like the trace of f*, and
L = ∑i (−1)i ni , the Lefschetz number ;
    The theorem states that this number can also be obtained as a sum of
    contributions of all the fixed points of f.
  * Relationships: It is
    like a finite (as opposed to infinitesimal) generalization of the
    concept of Euler characteristic.
  * Example: Consider the
    inversion map on S2, A:
    S2 → S2;
    We know that this does not have any fixed points;
    H0 = \(\mathbb R\),
    H1 = 0,
    H2  = \(\mathbb R\),
    and
L = ∑i (−1)i ni = 1 · 1 + (−1) · 0 + 1 · (−1) = 0 ;
    If the map had been orientation-preserving, there would have been
    fixed points and L ≠ 0.
  * Example: Every Lorentz
    transformation fixes at least one null direction.
  @ References: van Lon MS-a1509
    [quantum mechanical path integral methods, and other index theorems].
Borel Fixed-Point Theorem
  $ Def: A connected
    solvable linear algebraic group over an algebraic closed field, when
    acting on a complete variety, has a fixed point.
  @ References: Borel AM(56).
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