Closed differential form

A differential form with vanishing exterior derivative: =0.
Closed differential form

Let MM be a and let ω\omega be a on MM. The notion of “closedness” is defined using the .

Definition

A form ωΩk(M)\omega\in\Omega^k(M) is closed if

dω=0. d\omega = 0.

The vector space of closed kk-forms is

Zk(M)ker ⁣(d:Ωk(M)Ωk+1(M)). Z^k(M) \coloneqq \ker\!\bigl(d:\Omega^k(M)\to\Omega^{k+1}(M)\bigr).

Closed forms are the “cocycles” in the complex (Ω(M),d)(\Omega^\ast(M),d); passing to cohomology by quotienting out yields the .

Basic facts

  • Every is closed: if ω=dη\omega=d\eta, then dω=d(dη)=0d\omega=d(d\eta)=0 because d2=0d^2=0.
  • Closedness is preserved by pullback: if F:MNF:M\to N is a and ω\omega is closed on NN, then the FωF^*\omega is closed on MM.

Examples

  1. Constant 1-forms on Rn\mathbb{R}^n.
    In standard coordinates, each dxidx^i is closed because d(dxi)=0d(dx^i)=0. Any constant-coefficient 1-form iaidxi\sum_i a_i\,dx^i is also closed.

  2. Standard symplectic form on R2n\mathbb{R}^{2n}.
    With coordinates (x1,y1,,xn,yn)(x_1,y_1,\dots,x_n,y_n), the 2-form

    ω0=i=1ndxidyi \omega_0=\sum_{i=1}^n dx_i\wedge dy_i

    is closed since d(dxi)=d(dyi)=0d(dx_i)=d(dy_i)=0 and dd satisfies the graded Leibniz rule.

  3. A closed but not exact 1-form on R2{0}\mathbb{R}^2\setminus\{0\}.
    On U=R2{0}U=\mathbb{R}^2\setminus\{0\} with coordinates (x,y)(x,y), the 1-form

    ω=ydx+xdyx2+y2 \omega=\frac{-y\,dx + x\,dy}{x^2+y^2}

    is closed (it is the “angular” form). It is not exact on UU, which can be detected by integrating ω\omega around the unit circle: the integral is nonzero, so ω\omega cannot be dηd\eta globally on UU.