Definition

Let EE and FF be smooth over the same MM. A linear differential operator of order at most mm is a

D:Γ(E)Γ(F)D:\Gamma^\infty(E)\longrightarrow\Gamma^\infty(F)

such that, in every coordinate neighborhood and bundle trivialization, it has the form

Ds=αmaααs,Ds=\sum_{|\alpha|\leq m}a_\alpha\,\partial^\alpha s,

where each aαa_\alpha is a smooth bundle-homomorphism-valued coefficient. The least such mm is the order of DD. Thus D(s)(x)D(s)(x) depends only on the mm-jet of ss at xx, not on values of ss away from xx.

Intrinsic characterization

For fC(M)f\in C^\infty(M), let MfM_f denote multiplication by ff and set adMf(D)=[D,Mf]\operatorname{ad}_{M_f}(D)=[D,M_f]. The operator DD has order at most mm exactly when every (m+1)(m+1)-fold iterated commutator vanishes:

adMfmadMf0(D)=0.\operatorname{ad}_{M_{f_m}}\cdots\operatorname{ad}_{M_{f_0}}(D)=0.

This formulation is independent of coordinates and trivializations. Order-zero operators are precisely smooth bundle homomorphisms acting pointwise. These equivalent descriptions are developed in Wells, chapter IV.

Structure and examples

Orders add under composition: if D1D_1 and D2D_2 have orders at most m1m_1 and m2m_2, then D2D1D_2D_1 has order at most m1+m2m_1+m_2. A is first order, while a connection Laplacian is second order. The leading-order coefficients assemble into the , which controls .

Conventions and scope
References
  1. R. O. Wells Jr., Differential Analysis on Complex Manifolds, 3rd ed., Springer, 2008. Publisher record. Relevant: chapter IV, differential operators and symbols.
  2. H. B. Lawson Jr. and M.-L. Michelsohn, Spin Geometry, Princeton University Press, 1989. Publisher record. Relevant: chapter III, differential operators on vector bundles.