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wood
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Homework Statement
Is the gaussian
$$\sqrt{\frac{\pi}{2\alpha}}e^{-\alpha x^{2}}$$
an eigenfunction of ## \widehat{T} = \frac{\hat{p}^{2}}{2m}## ? If so, what is the corresponding eigenvalue? If not, find a P.E. operator ##\widehat{U} = U(\hat{x}) ## which gives rise to a Hamiltonian ##\widehat{H}## for which this Gaussian is an energy eigenfunction. What physical system are we talking about?
Find the uncertainty in ##\Delta x##.
Homework Equations
$$\hat{p} = \frac{\hbar}{i}\frac{\partial}{\partial x}$$
time independent Schrodinger equation
##\{-\frac{\hbar^{2}}{2m} \frac{\partial^{2}}{\partial x^{2}}+U(x)\}\psi_n(x)=E_n\psi_n(x)##
The Attempt at a Solution
I have worked out the relative derivatives and determined that it isn't an eigenfunction.
##\widehat{T}\psi(x)= -\frac{\hbar}{2m} 2\alpha e^{-\alpha x^{2}}(2\alpha x^{2} -1)##
Then I plug all that into the TISE and solve for ##\widehat{U}## and get
##\widehat{U}=\frac {\hbar^{2} + 4\alpha^{2}x^{2}}{2m}##
Hopefully I am correct up to here.
Now I am asked to find ##\Delta x ##
I think I need
## \Delta x= \sqrt{ \langle x^{2} \rangle - \langle x \rangle^{2}}##
where
## \langle x \rangle = \int_{-\infty}^\infty x|\psi|^{2} \,\mathrm{d}x##
which gives me 0
but I get confused here where I think I need
## \langle x^{2} \rangle = \int_{-\infty}^\infty x^{2}|\psi|^{2} \,\mathrm{d}x##
is the x2 term just the square of my function? So in principal I am just multiplying the square of my function by the mod of the function squared? THen taking the integral?
Thanks
edit :- sorted formatting of equation
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