For a f:URnRmf:U\subseteq\mathbb R^n\to\mathbb R^m, its Cartesian kk-jet at aUa\in U is the array

jakf=(αf(a))αk.j_a^k f=(\partial^\alpha f(a))_{|\alpha|\le k}.

Here α\alpha is a . Two functions have the same kk-jet when all these derivative values agree. The same data can be encoded by the polynomial

αkαf(a)α!(xa)α.\sum_{|\alpha|\le k}\frac{\partial^\alpha f(a)}{\alpha!}(x-a)^\alpha.
Infinite jets and coordinate choices

An infinite jet specifies these values for every order; it does not assert convergence of the associated formal Taylor series. Cartesian jets use fixed Euclidean coordinates. The is the corresponding coordinate-independent geometric construction.