Differential Forms |
In General
> s.a. exterior algebra and calculus;
integration on manifolds.
* Idea: Antisymmetric tensors,
for which Cartan developed a special formalism, terminology and notation.
$ Def: A \(p\)-form is
a totally antisymmetric covariant tensor field of order \(p\).
* Notation: The space of
one-forms on M is usually denoted by T*\(M\), that of \(p\)-forms
by Λp T*M,
ΛpM or
ΩpM.
* Chiral p-forms:
Abelian p-form potentials with self-dual field strengths.
* And other structure:
Forms are a submodule of the algebra of all tensor fields on M;
Together with the exterior product, this forms the exterior algebra or
Grassmann algebra of M; dim \(\Lambda^p{}_x(M) = n!/p!(n-p)!\)
@ General references: Flanders 63;
Cartan 67;
Von Westenholz 81;
Bott & Tu 82;
Darling 94;
Jancewicz gq/98 [visualization];
Morita 01 [geometry];
Ivancevic & Ivancevic a0807-ln;
Lessig a1206 [primer];
Guillemin & Haine 19.
@ Related topics: in de Rham 60 [of odd kind];
Hitchin m.DG/00 [3-forms in 6D and 7D];
> s.a. grassmann structures;
types of cohomology theories.
@ Chiral p-forms: Bengtsson & Kleppe IJMPA(97)ht/96;
Pasti et al PRD(97) [covariant actions];
Bonetti et al PLB(13) [Kaluza-Klein inspired action];
Buratti et al PLB(19)-a1909
[self-interacting chiral 2n-form in 4n+2 dimensions, Lagrangian].
@ And electrodynamics: Schleifer AJP(83)dec;
Dappiaggi et al a1908 [manifold with timelike boundary];
Fumeron et al a2009 [in the classroom]
@ And other physics:
Petrova mp/01 [conservation laws],
mp/05 [equations of mathematical physics];
Rodrigues AFLB(07)-a0712 [detailed];
Perot & Zusi JCP(14) [review];
Alfaro & Riquelme PRD(14)-a1402 [bosonic (p–1)-forms as surces of torsion];
Estabrook a1405/JMP [for field theories];
Dray 14 [and general relativity];
Pommaret a1707 [in mathematical physics];
> s.a. field theories; lattice field theory.
(Hodge) Dual
$ Def: Given a p-form f on
an n-manifold M with volume form ε and metric g
(with p ≤ n), its dual is the (n−p)-form
*fc.. d := (1/p!) f a.. b εa.. bc.. d .
* Properties: It follows that **f
= (−1)s+p(n−p)
f.
* For a curvature tensor:
The left and right duals are, respectively,
*Rabcd := \(1\over2\)εabmn Rmncd and R*abcd:= \(1\over2\)Rabmn εmncd .
* And physics: The duality operation
applied to the electromagnetic (Faraday) field tensor (2-form) interchanges the electric
and magnetic fields; > s.a. duality.
@ And conformal structure: Dray et al JMP(89);
Harnett JMP(91).
@ Related topics: Saa JGP(95) [for affine manifold with torsion];
Klinker JGP(11) [generalized definition];
Sen a1903 [self-dual forms, dynamics].
Volume Form > s.a. types of field theories.
$ Def: For an n-dimensional
manifold M, a nowhere-vanishing n-form ω.
* And connections: A volume
form is compatible with a connection if for all X ∈ TM,
\(\cal L\)X ω =
(Da Xa)
ω (for the divergence theorem to apply).
* Example: The volume
form ε defined by a metric g is ε =
|g|1/2 dx1
∧ ... ∧ dxn;
It is compatible with the Christoffel symbols, but not with a Riemann-Cartan
connection, \(\cal L\)X
ω = (Da
Xa −
2 Ta
Xa)
ω, where Ta:=
Tbab.
@ General references:
Cartier et al in(01)mp/00 [characterization].
@ As a dynamical variable:
Guendelman & Kaganovich a0811-conf;
Guendelman et al a1505-conf,
Benisty et al a1905-conf [in gravity and cosmology];
Benisty et EPJP-a2006
[non-canonical volume forms and modified gravity, rev].
Lie-Algebra Valued Forms
* Canonical form: Given
a Lie group G, the canonical (Maurer-Cartan) form on G
is the Lie-algebra-valued 1-form ω: TG →
\(\cal G\) = TeG
defined by ω(vg)
= Lg−1'
vg; Theorem:
Rg* ω =
Ad(g−1) · ω.
* Maurer-Cartan structure equation:
If {θI} is a basis for the
dual \(\cal G\)* of the Lie algebra of a group G, i.e. for the left-invariant
1-forms on G, then
dθI = −\(1\over2\)CIJK θJ ∧ θK .
Other Special Types and Generalizations > s.a. deformation
quantization; Star Product; superspace.
* Closed form: A form
ω whose exterior derivative vanishes, dω = 0.
* Exact form: A form
ω which can be expressed as the exterior derivative
of another form, ω = dθ.
* Poincaré's lemma:
On a contractible space, any closed form is exact (e.g., not in
\({\mathbb R}^2\setminus\{0\}\), non-contractible).
@ General references: in Flanders 63;
in Nash & Sen 83.
@ Closed forms: Torre CQG(95)gq/94 [classification];
Farber 04;
Farber & Schütz Top(06) [closed 1-forms with at most one zero];
Burns a1906
[generalization of Poincaré lemma to divergence-free multivector fields].
@ Fractional order:
Cottrill-Shepherd & Naber JMP(01)mp/03,
mp/03;
Tarasov JPA(05).
@ Discrete:
Richter et al CQG(07)gq/06 [and spherical symmetry in general relativity];
Dowker JGP(07) [on sphere tessellations];
Dolotin et al TMP(08)-a0704 [based on simplicial complexes];
Richter & Frauendiener JSC(10)-a0805 [Gowdy solutions, numerical].
@ Other generalizations:
Nurowski & Robinson CQG(01) [and spacetime geometry];
Robinson IJTP(03) [and gauge theories],
JMP(03) [and general relativity],
JPA(07) [rev, and applications],
CQG(09)
[integral calculus, Stokes' theorem, Chern-Simons and Einstein-Yang-Mills theories];
Chatterjee et al IJGMP(08)-a0706 [negative forms, and path-space forms];
Gallego Torromé a1207
[higher-order, and applications to electrodynamics];
Robinson a1312 [and gravitation];
> s.a. clifford calculus;
formulations of electromagnetism [pair and impair].
@ Related topics: Frauendiener talk(03).
main page
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send feedback and suggestions to bombelli at olemiss.edu – modified 26 dec 2020