1. For an electron in the ground state of a hydrogen atom potential, calculate the expectation value of:
a) 1/r
b) r
c) x^2
d) the vector r = (x,y,z)
e) p^2
[what is the relationship between the expectation value of r and of x^2 ?
2. a) (Using your results from problem 1) what are the expectation values of the K.E. and potential energy, respectively. Calculate your answer in e.V. and make sure the signs are correct.
How does the K.E. compare with the P.E.? (xc) How does this relate to the virial theorem?
b) Show that the P.E. can be expressed very simply using e^2 and the characteristic length scale, a_0 = hbar^2/m e^2.
c) Show that your result for the K.E. can be expressed very simply using hbar, m and the characteristic length scale, a_0 = hbar^2/m e^2.
d) why does this make sense?
3. For many potentials, there is no intrinsic length scale associated with V(r) and yet there can be quantum length scale which emerges when a particle of mass m is localized by the potential. What are the characteristic length scales for each of the following?:
a) V(x)= -alpha delta(x)
b) V(x) = (1/2) k x^2
c) V(x) = -e^2/r (3D)
4. Using the Psi_n,l,m as a basis, what is the represention of the state Psi = A (x/2a_0) exp[-r/2a_0], where A is a normalization constant independent of r, theta and phi or x, y and z). In other words, write the state Psi = A (x/2a_0) exp[-r/2a_0] as a linear combination of Psi_n,l,m eigenstates. How many states do you need? Is this a mixed state?
5. For the 3D H.O., the 1st excited state manifold contains 3 states: which could be called 100,
010, 001; where 100 includes a term proportional to x, 010 includes a term proportional to y, ...
Show, by construction, that the 1st-excited state manifold of H can be arranged to also include real eigenstate which are proportional to x, y and z (and orthogonal to each other). What else does the 1st excited state manifold of H include? Discuss the differences and similarities of the 1st excited state manifolds of H and a symmetric 3DH.O..
6. a) Use appropriate indentities and relationships to express Psi3,2,2 + Psi3,2,-2 as a relatively simple function of the cartesian variables x, y and z.
b) Show that a 45 degree rotation of this state (around the z axis) will give another state that: is a linear combination of 2 Psi n,l,m states, and is a relatively simple function of x,y and z. What is the linear combination? What would be good names for these states?
7. Use that state from problem 4, let's call it Psi_2x, to make the state (Psi 100 + Psi_2x)/sqrt(2)
a) calculate the expectation value of x for an electron in this state? Is this a mixed state? Is x a function of time?
8. With or without doing any calculations (calculation is extra-credit of you have time), describe the nature of the trajectory of the expectation value of the vector r:
a) in the state: (Psi 100 + Psi 211)/ sqrt(2)
b) in the state: (Psi 100 + Psi 210)/ sqrt(2)
c) Are these qualitatively similar or different? Discuss?
9. a) What is the degeneracy of the 2nd excited state (manifold) of a symmetric 2-D H.O. ?
(extra credit) b) What angular momentum eigenstates are contained within this N-dimensional subspace?
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(extra credit) a) Figure out how to make the state, B (x^2 - y^2) exp[-r/3a_0] from a combination of Psi_n,l,m and/or how to make C x y exp[-r/3a_0].
b) What is the difference (relationship) between these two states? Are they eigenstates or not? Are they degenerate?
Thursday, May 28, 2009
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Well, I've kind of run into a wall on number 5, and just need some clarification.
ReplyDeleteIn generalizing the Harmonic Oscillator potential to 3D, using V(r)=1/2mw^2r^2, the angular part is similar, but there's some real nasty stuff for the radial part.
The extreme cases method isn't churning out a nice solution like for the H atom (at least for now). I'm wondering if their is a substitution trick here?
Jon, That would be a very hard way to do it and strongly NOT recommended. Instead, use products of the 1DHO eig. states. That is what the notation 100 means: 1st ex state for x multiplied by the gs for y multiplied by the gs for z.
ReplyDeleteAh.
ReplyDeleteSo we're looking for explicit proportionality to x, y, or z for the first excited states of the H atom.
Simply put, does this mean we must express the H atom's 200 state, which has a (1-r/2a_0) term, in terms of x,y,z? And similarly for 210, 211, and 21-1? Or am I just completely out of whack?
I get imaginary terms for 211 and 21-1 and the exponentials are different compared to the H.O., but it seems to work out.
There is no point in trying to rewrite the 200 state in terms of x,y,z. Work with the other (n=2) states.
ReplyDeleteRicky: nice comment
ReplyDeletewait... man down!
Jon: Swim back!
Ethan, Ricki and I get the following manifold
ReplyDeletePsi_2,1,-1 - Psi_2,1,1
-Psi_2,1,-2 - Psi_2,1,1
Psi_2,1,0
Psi_200
We think this is correct. However, we aren't yet seeing any obvious similarities between this and the 1st excited degeneracy manifold for the 3D H.O. Anyone have any ideas? Jon????
I'm getting that...
ReplyDeleteThe combination proportional to y is: i(psi_2,1,-1 - psi_2,1,1)
the combination proportional to x is:
psi_2,1,1 + psi_2,1,-1
and proportional to z is just
psi_2,1,0
using euler's formula (for the phi terms), and the definition of x y and z in spherical coordinates (in the back of our Griffiths EM book)
Oh. And does anyone know the equation for
ReplyDeletePsi_3,2,2 or Psi_3,2,-2 ?
Pg 455 in Liboff gives the radial components and pg 373 gives the angular component.
ReplyDeleteOh, cool. Thank you!
ReplyDeleteThis HW could be due either Thursday or Friday. Whichever you prefer. I will plan to hand it back at the Sunday review section.
ReplyDeleteA few of us a couple plots of the probability distributions of the two mixed states of Prob. 8 for a specified radius of 1 and leaving out a bunch of constants if anyone is interested. They are pretty trippy looking assuming we did them correctly. The time dependence for both results in these shapes rotating around the vertical axis.
ReplyDelete|Psi_100 + Psi_211|^2
people.ucsc.edu/~jkcarman/Images/HW9_100+211.pdf
|Psi_100 + Psi_210|^2
people.ucsc.edu/~jkcarman/Images/HW9_100+210.pdf
I animated my result for the first part of problem 8:
ReplyDeletehttp://people.ucsc.edu/~akunapul/animate.gif
It looks like a rotating bean bag.
And here's the 2nd one:
ReplyDeletehttp://people.ucsc.edu/~akunapul/animate2.gif