The simplest model for a local deterministic physical theory is a field function i.e. a function defined at each space time coordinate whose evolution is determined by the previous field values in the immediate neighborhood. The starting point for any theory like this must be the classical wave equation
for that equation is universal in physics describing both electromagnetic effects and the relativistic quantum wave function (Klein Gordon equation ) for the photon.
By `discretized' I mean an equation that is modified to map integers to integers. A modification is required because there is no finite difference approximation to the wave equation that can do this. The universality of the wave function requires that any discrete model for physics approximates this continuous model to extraordinary accuracy. Discretizing the finite difference equation adds a rich combinatorial structure that has a number of properties that suggest quantum mechanical effects. Perhaps the most obvious is that an initial disturbance cannot spread out or diffuse indefinitely as it does with the continuous equation. It must either diverge and fill all of space with increasing energy or break up into independent structures that will continue to move apart, i.e., become quantized.
We describe how to approximate the wave equation
with a discretized finite difference
equation.
Let P be defined at each point in a 4 dimensional grid.
To simplify the expression for
we will adopt the following
conventions. Subscripts will be written relative to
and
will be dropped if they are the same as this point. Thus
is at the same position in the previous time step.
is
at the same time step and z coordinate and one position less on
both the x and y axes.
The wave equation is approximated by the difference equation:

The difference equation discretizes space and
time but not the function
defined on this discrete manifold.
The simplest approach to discretizing
the function values is to constrain
them to be integers. This requires
either that
be an integer or
that some rounding scheme be employed
that forces the product
involving
to be an integer.
The former is not possible since
it does not allow for solutions that
approximate the differential equation.
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