For a f:U⊆Rn→Rmf:U\subseteq\mathbb R^n\to\mathbb R^m, its Cartesian kk-jet at a∈Ua\in U is the array

jakf=(∂αf(a))∣α∣≤k.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

∑∣α∣≤k∂αf(a)α!(x−a)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.