Find the eigenfunctions and eigenvalues of the position operator.
Find the eigenfunctions and eigenvalues of the position operator.
Let g_y(x) be the eigenfunction and y the eigenvalue:
\widehat{x} g_{y}(x)=x g_{y}(x)=y g_{y}(x) (3.37)
Here y is a fixed number (for any given eigenfunction), but x is a continuous variable. What function of x has the property that multiplying it by x is the same as multiplying it by the constant y? Obviously it’s got to be zero, except at the one point x=y ; in fact, it is nothing but the Dirac delta function:
g_{y}(x)=A\delta (x-y)
This time the eigenvalue has to be real; the eigenfunctions are not square integrable, but again they admit Dirac orthonormality:
\int_{-\infty }^{\infty }{g^{*}_{\acute{y} }(x) g_{y} (x) } dx=\left|A\right|^{2} \int_{-\infty } ^{\infty } {\delta (x-\acute{y})\delta (x-y)}dx= \left|A \right |^{2}\delta (y-\acute{y}) (3.38)
If we pick A=1 , so
g_{y}(x)=\delta (x-y) (3.39)
then
\left\langle g_{\acute{y}}|g_{y}\right\rangle \delta (y-\acute{y}) (3.40)
These eigenfunctions are also complete:
f(x)=\int_{-\infty }^{\infty }c(y){g_{y}(x)} dy=\int_{-\infty }^{\infty }{c(y)\delta (x-y)}dy (3.41)
with
c(y)=f(y) (3.42)
(trivial, in this case, but you can get it from Fourier’s trick if you insist).