|  Integration on Manifolds | 
In General
  > s.a. differential forms; lie groups.
  * Idea: Integration on
    an n-manifold (without a metric, with just an orientation)
    is defined only for n-forms, by
∫U fa... b:= ∫U f(x) dnx , sometimes written ∫U fa... b dva... b ,
where U has to be covered by one (right-handed) coordinate chart (otherwise we generalize the definition using partitions of unity) and
fa... b = f(x) (dx1 ∧ ... ∧ dxn)a... b .
* For functions: Choose a volume element or measure (which could be defined by a metric), and define
∫U f (dnv):= ∫U f εa... b .
  * For other objects: Need even more
    structure, except for some integrals over lower-dimensional submanifolds.
  @ In curved spacetime, for general relativity:
    DeBenedictis phy/98.
On Submanifolds
  * Idea: Given a p-dimensional
    submanifold Σ in an n-dimensional manifold M, the natural things
    to integrate there are p-forms, but we could integrate on Σ an n-form
    f defined on M by defining the result to be the integral of the p-form
    φ*f, where φ is the embedding φ: Σ →
    M.
  * Notation: An integral over
    a p-submanifold S can be indicated in one of two ways,
∫S Aa... b dva... b , or ∫S Bm... n dSm... n ,
where A is a p-form on S and B an (n−p)-th rank tensor with indices normal to S.
Stokes' Theorem
  > s.a. Gauss' Theorem; holonomy
  [for Levi-Civita connection, and curvature]; Wilson Loop.
  * In 3D space:
∫S ∇ × A · ds = ∫∂(S) A · dl ; 2 ∫S ∇a Ab dvab = ∫∂(S) Aa dva ; ∫V ∇ · A d3v = ∫∂(V) A · ds .
* In general:
∫U dω = ∫∂(U) ω , from which ∫U ∇a va = ∫∂(U) va εab...c = ∫∂(U) va na ;
    Special cases are the 3D version, Gauss' theorem, and the Green identities
    (> see vector calculus).
  * For a rank-two (antisymmetric) tensor:
\(\int_S\) ∇a T [ab] dSb = \(-{1\over2}\int_{\partial S}\) T [ab] dSab .
  @ General references: in Flanders 63;
    Saslow EJP(07) [computationally based proof].
  @ Generalized: Bralic ht/93 ["surfaceless"];
    Mensky PLA(04)gq [in terms of path group in Minkowski space];
    Meunier EJC(08) [combinatorial].
  @ Non-abelian: Diakonov & Petrov hl/00,
    JETP(01)ht/00 [including Yang-Mills and gravity];
    Kondo ht/00-proc [Wilson loops];
    Broda in(01)mp/00;
    Broda & Duniec mp/01 [Wilson loops];
    Mensky gq/02-conf [in terms of path group in Minkowski];
    Matsudo & Kondo PRD(15)-a1509 [and implications for quark confinement];
    > s.a. loops [gauge theories and loop variables];
      path integrals for gauge theories.
  > Online resources:
    see Wikipedia page.
 Specific Results and Types of Manifolds > s.a. lie groups
  and examples; Reynolds Theorem.
  @ References: Hannay & Nye JPA(04) [2-sphere, Fibonacci numerical integration];
    Somogyi JMP(11)-a1101 [angular integrals in d dimensions];
    Felder & Kazhdan a1608 [regularization of divergent integrals].
Generalizations
  @ Generalized integrals: Yekutieli 15 [non-abelian multiplicative integration on surfaces].
  > Generalized manifolds:
    see differential geometry; fractals;
    grassmann; operator theory;
    Supermanifolds.
 main page
  – abbreviations
  – journals – comments
  – other sites – acknowledgements
  send feedback and suggestions to bombelli at olemiss.edu – modified 10 apr 2020