Dixanadu
- 250
- 2
Homework Statement
Hey guys, so here's the question:
The energy eigenstates of the hydrogen atom \psi_{n,l,m} are orthonormal and labeled by three quantum numbers: the principle quantum number n and the orbital angular momentum eigenvalues l and m. Consider the state of a hydrogen atom at t=0 given by a linear combination of states:
\Psi=\frac{1}{3}(2\psi_{0,0,0}+2\psi_{2,1,0}+\psi_{3,2,2})
(a) What is the probability to find in a measurement of energy E_{1}, E_{2}, E_{3}?
(b) Find the expectation values of the energy \vec{\hat{L}}^{2} and L_{z}.
(c) Does this state have definite parity? (HINT: use orthonormality of the \psi_{n,l,m} and the known eigenvalues of \psi_{n,l,m} with respect to \hat{H}, \vec{\hat{L}}^{2}, \hat{L}_{z}.
Homework Equations
So here's what we need I think:
Eigenvalues of \vec{\hat{L}}^{2} = \hbar^{2}l(l+1)
Eigenvalues of \hat{L}_{z} = \hbar m
Eigenvalues of \hat{H} = E_{n}..right?
The Attempt at a Solution
so for part (a)...is this just really trivial, that the E_{1}=\frac{2}{3}, E_{2}=\frac{2}{3}, E_{3}=\frac{1}{3} or am I missing something?
(b) I've got something pretty weird...like <\vec{\hat{L}}^{2}>=\frac{8}{3}\hbar^{2} and <\hat{L}_{z}>=\frac{2}{3}\hbar which doesn't seem right to me...
(c) I have no idea!
could you guys gimme a hand please?
thanks a lot!