|> In Bjorken and Drell - QED part 1 I read a statement that one doesnt
|> use a square rooted Hamiltonian (H= SQRT/m*2.c*4+m*2.p*2/) in a wave
[quoted text clipped - 6 lines]
|> than the n-th derivative √ in the end all is taken to the limit of the
|> local point)
It is not n+1 versus n but N_large versus n = 1 here. Think of finite
differences. With n = 1 you communicate with neighboring grid points.
With n = 1 applied N times you communicate with grid points a count N
away. Now let N --> \infty.
|> 2.Then in the quantum theory based on Schroedinger equation there are
|> only second order derivatives over space but nevertheless one is left
|> at the end with a non-local theory (EPR type paradoxes).
Here, think about elliptic equations.

Signature
cu,
Bruce
drift wave turbulence: http://www.rzg.mpg.de/~bds/
tadchem - 23 Mar 2005 20:00 GMT
> |> In Bjorken and Drell - QED part 1 I read a statement that one doesnt
> |> use a square rooted Hamiltonian (H= SQRT/m*2.c*4+m*2.p*2/) in a wave
[quoted text clipped - 11 lines]
> With n = 1 applied N times you communicate with grid points a count N
> away. Now let N --> \infty.
Personally I would suggest a transformation of coordinate systems to
something in which your square root is a little more well-behaved,
possibly a rotation with renormalization.
Tom Davidson
Richmond, VA