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MathematicalPhysicist
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Homework Statement
With the wave function [tex]\psi(r)[/tex] of a particle, one forms the function:
[tex]D(R,P)=\frac{\int exp(-\frac{i}{\hbar} P\cdot r)\psi^*(R-r/2)\psi (R+r/2) dr}{(2\pi \hbar)^3}[/tex], which is the density in phase of a classical statistical mixture associated with this wave function, Show that:
1. [tex]\int D(R,P)dP=|\psi (R)|^2[/tex] [tex]\int D(R,P)dR=|\psi (P)|^2[/tex].
2. if the particle is free, the evolution in time of the mixture is strictly that of a statistical mixture of free classical particles of the same mass;
3. find the spreading law of a free wave packet.
Homework Equations
I think one of them is dirac delta function:
[tex]\int \frac{exp(-\frac{i}{\hbar} P\cdot r)}{(2\pi \hbar)^3}dr=\delta(r) \ \int \frac{exp(-\frac{i}{\hbar} P\cdot r)}{(2\pi \hbar)^3}dP=\delta(P)[/tex]
The Attempt at a Solution
1. So far by using the above equality I get that:
[tex]\int D(R,P)dP=\int \frac{\int exp(-\frac{i}{\hbar} P\cdot r)\psi^*(R-r/2)\psi (R+r/2) dr}{(2\pi \hbar)^3} dP=\int \psi^*(R-r/2)\psi (R+r/2) dr[/tex], I don't see how this becomes the amplitude of the wave function in the R space squared?
2. Don't know what I need to show here.
3. The same as with 2.
Any hints?
Not answers!
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