On Sat, Aug 17, 2019 at 10:28 AM smitra <[email protected]> wrote:

> On 16-08-2019 09:01, Bruce Kellett wrote:
> > On Fri, Aug 16, 2019 at 4:43 PM smitra <[email protected]> wrote:
> >
> >
> > I think you need to prove that. In my understanding, A(x) = <x|A> is
> > to be interpreted as the amplitude for a wave through slit A to get to
> > the screen at x. There is nothing 3-dimensional about this. The 'x' is
> > just the distance from the centre of the screen in the plane of the
> > screen. Nothing else is relevant. You do not have to integrate over
> > all space because you use a complete set of states in the x-direction:
> >  int |x><x| dx = 1.
>
> A quantum state is defined in the position representation by assigning
> an amplitude to all points in space. It can be the case that the
> amplitude is zero outside of a narrow volume surrounding the the screen,
> in which case the integration can be approximated as an integral over
> the screen's surface.
>
> The orthogonality can be rigorously proved as follows. If we have a
> single particle incident on the two slits described by a time dependent
> wave function psi(x,t) = 1/sqrt(2) [A(x,t) + B(x,t)] such that at A(x,0)
> is nonzero at one slit and B(x,0) at the other slit, then A(x,0) and
> B(x,0) are obviously orthogonal. Since time evolution will preserve
> inner products, A(x,t) and B(x,t) will remain orthogonal as a function
> of t. One can then describe the interaction with the screen as an
> effective collapse that will happen with the largest probability when
> the peak of the wavefunction has arrived at the screen.
>

The slits are orthogonal only if they are eigensatates of the position
operator (in the x direction). That is the case only if you have a
measurement that gives which-way information. Then there is no
interference, as advertised. The amplitudes at the slits aren't orthogonal
just because you say so.

Bruce

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