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In mathematics, the Cauchy–Kowalevski theorem is the main local existence and uniqueness theorem for analytic partial differential equations associated with Cauchy initial value problems. A special case was proved by Augustin Cauchy (1842), and the full result by Sophie Kowalevski (1875).

Contents

[edit] First order Cauchy–Kovalevski theorem

Let V and W be finite-dimensional vector spaces, with n = dim W. Let A1, ..., An−1 be analytic functions with values in End (V) and b an analytic function with values in V, defined on some neighbourhood of (0,0) in V x W. Then there is a neighbourhood of 0 in W on which the quasilinear Cauchy problem

 f_{x_n} = A_1(x,f) f_{x_1} + \dots + A_{n-1}(x,f)f_{x_{n-1}} + b(x,f)

with initial condition

f(x) = 0 on the hypersurface xn = 0

has a unique analytic solution  f: V \rightarrow W near 0.

The theorem and its proof are valid for analytic functions of either real or complex variables. Lewy's example shows that the theorem is not valid for all smooth functions.

[edit] Proof by analytic majorization

Both sides of the partial differential equation can be expanded as formal power series and give recurrence relations for the coefficients of the formal power series for f that uniquely determine the coefficients. The Taylor series coefficients of the Ai's and b are majorized in matrix and vector norm by a simple scalar rational analytic function. The corresponding scalar Cauchy problem involving this function instead of the Ai's and b has an explicit local analytic solution. The absolute values of its coefficients majorize the norms of those of the original problem; so the formal power series solution must converge where the scalar solution converges.

[edit] Higher-order Cauchy–Kovalevski theorem

If F and fj are analytic functions near 0, then the non-linear Cauchy problem

 \partial_t^k h = F\left(x,t,\partial_t^j\,\partial_x^\alpha h \right),\text{ where }j<k\text{ and }|\alpha|+j\le k,\,

with initial conditions

 \partial_t^j h(x,0) = f_j(x),\qquad 0\le j<k,

has a unique analytic solution near 0.

This follows from the first order problem by considering the derivatives of h appearing on the right hand side as components of a vector-valued function.

[edit] Example

The heat equation

 \partial_t h = \partial_x^2 h \,

with the condition

h(0,x) = {1\over 1+x^2}\text{ for }t = 0 \,

has a unique formal power series solution (expanded around (0, 0)). However this formal power series does not converge for any non-zero values of t, so there are no analytic solutions in a neighborhood of the origin. This shows that the condition |α| + j ≤ k above cannot be dropped. (This example is due to Kowalevski.)

[edit] References

[edit] External links




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