In mathematics, Carathéodory's existence theorem says that an ordinary differential equation has a solution under relatively mild conditions. It is a generalization of Peano's existence theorem. Peano's theorem requires that the right-hand side of the differential equation be continuous, while Carathéodory's theorem shows existence of solutions (in a more general sense) for some discontinuous equations. The theorem is named after Constantin Carathéodory.
Consider the differential equation
                              y          ′                (        t        )        =        f        (        t        ,        y        (        t        )        )                        with initial condition
                    y        (                  t                      0                          )        =                  y                      0                          ,                        where the function ƒ is defined on a rectangular domain of the form
                    R        =        {        (        t        ,        y        )        ∈                  R                ×                              R                                n                                  :                          |                t        −                  t                      0                                    |                ≤        a        ,                  |                y        −                  y                      0                                    |                ≤        b        }        .                Peano's existence theorem states that if ƒ is continuous, then the differential equation has at least one solution in a neighbourhood of the initial condition.
However, it is also possible to consider differential equations with a discontinuous right-hand side, like the equation
                              y          ′                (        t        )        =        H        (        t        )        ,                y        (        0        )        =        0        ,                where H denotes the Heaviside function defined by
                    H        (        t        )        =                              {                                                            0                  ,                                                                      if                                     t                  ≤                  0                  ;                                                                              1                  ,                                                                      if                                     t                  >                  0.                                                                                        It makes sense to consider the ramp function
                    y        (        t        )        =                  ∫                      0                                t                          H        (        s        )                          d                s        =                              {                                                            0                  ,                                                                      if                                     t                  ≤                  0                  ;                                                                              t                  ,                                                                      if                                     t                  >                  0                                                                                        as a solution of the differential equation. Strictly speaking though, it does not satisfy the differential equation at                     t        =        0                , because the function is not differentiable there. This suggests that the idea of a solution be extended to allow for solutions that are not everywhere differentiable, thus motivating the following definition.
A function y is called a solution in the extended sense of the differential equation                               y          ′                =        f        (        t        ,        y        )                 with initial condition                     y        (                  t                      0                          )        =                  y                      0                                   if y is absolutely continuous, y satisfies the differential equation almost everywhere and y satisfies the initial condition. The absolute continuity of y implies that its derivative exists almost everywhere.
Consider the differential equation
                              y          ′                (        t        )        =        f        (        t        ,        y        (        t        )        )        ,                y        (                  t                      0                          )        =                  y                      0                          ,                        with                     f                 defined on the rectangular domain                     R        =        {        (        t        ,        y        )                          |                                  |                t        −                  t                      0                                    |                ≤        a        ,                  |                y        −                  y                      0                                    |                ≤        b        }                . If the function                     f                 satisfies the following three conditions:
                    f        (        t        ,        y        )                 is continuous in                     y                 for each fixed                     t                ,                    f        (        t        ,        y        )                 is measurable in                     t                 for each fixed                     y                ,there is a Lebesgue-integrable function                     m        (        t        )                ,                               |                t        −                  t                      0                                    |                ≤        a                , such that                               |                f        (        t        ,        y        )                  |                ≤        m        (        t        )                 for all                     (        t        ,        y        )        ∈        R                ,then the differential equation has a solution in the extended sense in a neighborhood of the initial condition.
A mapping                     f        :        R        →                              R                                n                                   is said to satisfy the Carathéodory conditions on                     R                 if it fulfills the condition of the theorem.
Assume that the mapping                     f                 satisfies the Carathéodory conditions on                     R                 and there is a Lebesgue-integrable function                     k        (        t        )                ,                               |                t        −                  t                      0                                    |                ≤        a                , such that
                              |                f        (        t        ,                  y                      1                          )        −        f        (        t        ,                  y                      2                          )                  |                ≤        k        (        t        )                  |                          y                      1                          −                  y                      2                                    |                ,                for all                     (        t        ,                  y                      1                          )        ∈        R        ,        (        t        ,                  y                      2                          )        ∈        R        .                 Then, there exists a unique solution                     y        (        t        )        =        y        (        t        ,                  t                      0                          ,                  y                      0                          )                 to the initial value problem
                              y          ′                (        t        )        =        f        (        t        ,        y        (        t        )        )        ,                y        (                  t                      0                          )        =                  y                      0                          .                Moreover, if the mapping                     f                 is defined on the whole space                               R                ×                              R                                n                                   and if for any initial condition                     (                  t                      0                          ,                  y                      0                          )        ∈                  R                ×                              R                                n                                  , there exists a compact rectangular domain                               R                      (                          t                              0                                      ,                          y                              0                                      )                          ⊂                  R                ×                              R                                n                                   such that the mapping                     f                 satisfies all conditions from above on                               R                      (                          t                              0                                      ,                          y                              0                                      )                                  . Then, the domain                     E        ⊂                              R                                2            +            n                                   of definition of the function                     y        (        t        ,                  t                      0                          ,                  y                      0                          )                 is open and                     y        (        t        ,                  t                      0                          ,                  y                      0                          )                 is continuous on                     E                .
Consider a linear initial value problem of the form
                              y          ′                (        t        )        =        A        (        t        )        y        (        t        )        +        b        (        t        )        ,                y        (                  t                      0                          )        =                  y                      0                          .                Here, the components of the matrix-valued mapping                     A        :                  R                →                              R                                n            ×            n                                   and of the inhomogeneity                     b        :                  R                →                              R                                n                                   are assumed to be integrable on every finite interval. Then, the right hand side of the differential equation satisfies the Carathéodory conditions and there exists a unique solution to the initial value problem.