Let π:E→M\pi:E\to M be a smooth of rank rr over a . For an integer k≥0k\ge 0, the k-th symmetric power bundle of EE is the vector bundle

SkE→MS^k E \to M

defined fiberwise by

(SkE)x:=Sk(Ex),(S^k E)_x := S^k(E_x),

the kk-th symmetric power of the vector space ExE_x (i.e. the quotient of Ex⊗kE_x^{\otimes k} by the action of the symmetric group permuting factors).

In local frames, if (e1,…,er)(e_1,\dots,e_r) is a local frame of E∣UE|_U, then the symmetrized tensors built from the eie_i give a local frame of (SkE)∣U(S^kE)|_U. Under a change of frame with transition matrix gg, the induced transition on SkES^kE is the symmetric power representation SkgS^k g. This can be constructed systematically from the local description of the E⊗kE^{\otimes k}.

Functoriality holds: a Φ:E→F\Phi:E\to F over idM\mathrm{id}_M induces SkΦ:SkE→SkFS^k\Phi:S^kE\to S^kF fiberwise.

Examples
  1. Symmetric 2-tensors. For E=T∗ME=T^*M, the bundle S2T∗MS^2T^*M has sections given by symmetric covariant 2-tensor fields; a Riemannian metric is an everywhere positive-definite section of this bundle.
  1. . If L→ML\to M is a line bundle, then SkL≅L⊗kS^k L \cong L^{\otimes k} canonically (since there is no nontrivial symmetrization in rank 1).
  1. Trivial bundle case. If E≅M×FrE\cong M\times \mathbb F^r, then SkE≅M×Sk(Fr)S^kE\cong M\times S^k(\mathbb F^r).