The Cauchy-Kowalevski Theorem

AKA Cauchy-Kovalevskaya theorem
Given a Cauchy problem, the Cauchy–Kowalevski theorem states:
If all the functions Fi are analytic in some neighborhood of the point

(t0,x10,x20,,ϕj,k0,k1,,kn0,),

and if all the functions ϕj(k) are analytic in some neighborhood of the point

(x10,x20,,xn0),

then the Cauchy problem has a unique analytic solution in some neighborhood of the point

(t0,x10,x20,,xn0).

For better understanding, let's focus on the case of first order PDEs (see @olver1995equivalence):

Definition 15.1. A system of first order partial differential equations for functions u(x)=(u1(x),,uq(x)), x=(x1,,xp) is said to be in Kovalevskaya form if it has been solved for the derivatives of the u's with respect to one of the x's, say xp, so that

(15.1)uαxp=Δα(x,u(1)~),α=1,,q,

where the right hand side depends on x1,,xp (denoted as x) and u1,,uq, and the first order partial derivatives ujβ=uβ/xj for β=1,,q,j=1,,p1 (denoted as u(1)~).

The Cauchy-Kovalevskaya Theorem concerns the existence and uniqueness of solutions to the Cauchy problem for a system in Kovalevskaya form (15.1), with initial Cauchy data

(15.2)uα(x1,,xp1,x0p)=hα(x1,,xp1),i=1,,q,

prescribed on an open subset of the initial hypersurface {xxp=x0p}. The fact that the system can be solved for all the xp-derivatives means that this hypersurface is noncharacteristic (in a sense, it means that the hypersurface is transversal to the natural flow given by the PDE). The Cauchy problem for the system (15.1) is to find a (local) solution u(x) to the system satisfying the given Cauchy data.

Theorem 15.2. Let (15.1) be an analytic system of partial differential equations in Kovalevskaya form, and let hα(x1,,xp1) be analytic functions defined in a neighborhood of (x01,,x0p1). Then, in a neighborhood of x0=(x01,,x0p), there exists a unique analytic solution to the Cauchy problem consisting of (15.1) and initial data (15.2).