John's Equation | John Equation

John's equation is an ultrahyperbolic partial differential equation satisfied by the X-ray transform of a function. It is named after Fritz John.

Given a function with compact support the X-ray transform is the integral over all lines in . We will parameterise the lines by pairs of points, on each line and define as the ray transform where

Such functions are characterized by John's equations

which is proved by Fritz John for dimension three and by Kurusa for higher dimensions.

In three dimensional x-ray computerized tomography John's equation can be solved to fill in missing data, for example where the data is obtained from a point source traversing a curve, typically a helix.

More generally an ultrahyperbolic partial differential equation (a term coined by Richard Courant) is a second order partial differential equation of the form

$\sum\limits_{i,j=1}^{2n} a_{ij}\frac{\partial^2 u}{\partial x_i \partial x_j} + \sum\limits_{i=1}^{2n} b_i\frac{\partial u}{\partial x_i} + cu =0$

where, such that the quadratic form

can be reduced by a linear change of variables to the form

It is not possible to arbitrarily specify the value of the solution on a non-characteristic hypersurface. John's paper however does give examples of manifolds on which an arbitrary specification of u can be extended to a solution.

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