Exterior power bundle

The vector bundle whose fiber at each point is the k-th exterior power of the original fiber.
Exterior power bundle

Let π:EM\pi:E\to M be a smooth vector bundle of rank rr over a . For an integer kk with 0kr0\le k\le r, the k-th exterior power bundle of EE is the vector bundle

ΛkEM \Lambda^k E \to M

defined fiberwise by

(ΛkE)x:=Λk(Ex). (\Lambda^k E)_x := \Lambda^k(E_x).

If (e1,,er)(e_1,\dots,e_r) is a local frame of EUE|_U, then the wedge products

ei1eik(1i1<<ikr) e_{i_1}\wedge \cdots \wedge e_{i_k}\qquad (1\le i_1<\cdots<i_k\le r)

form a local frame of (ΛkE)U(\Lambda^k E)|_U. Under a change of local frame with transition matrix g:UVGL(r,F)g:U\cap V\to \mathrm{GL}(r,\mathbb F), the induced transition matrix on ΛkE\Lambda^kE is the kk-th exterior power representation Λkg\Lambda^k g.

The construction is functorial: a Φ:EF\Phi:E\to F over idM\mathrm{id}_M induces ΛkΦ:ΛkEΛkF\Lambda^k\Phi:\Lambda^kE\to \Lambda^kF fiberwise.

This exterior-power construction is compatible with the viewpoint via universal properties.

Examples

  1. Forms as sections. Taking E=TME=T^*M, the sections of ΛkTM\Lambda^k T^*M are precisely smooth on MM.

  2. Determinant line bundle. For a rank rr bundle EE, the top exterior power ΛrE\Lambda^r E is a line bundle, often denoted det(E)\det(E). An of a real bundle can be encoded as a choice of “positive” component in det(E){0}\det(E)\setminus\{0\}.

  3. Low-degree cases. Λ0E\Lambda^0E is canonically the trivial line bundle M×FM\times \mathbb F, and Λ1EE\Lambda^1E\cong E canonically.