PHYS 424 Final Exam

December 16, 2002

Ñ2 = (1/r2)/r (r2/r) + 1/(r2sinq) /q (sinq /q) + 1/(r2 sin2q) 2/f2

Y00 = 1/sqrt(4p)
Y10 = sqrt[3/(4p)] cos(q)
Y1-1 = + sqrt[3/(8p)] sin(q) e -if       Y11 = - sqrt[3/(8p)] sin(q) e +if

2 sin A sin B = cos(A+B) - cos(A-B) and 2 cos A cos B = cos(A+B) + cos(A-B) ].

 

1. Consider a particle of mass m that is free to move in a one-dimensional region of length L that closes on itself (for instance, a bead which slides frictionlessly on a circular wire of circumference L.

(a) Show carefully that the states |n> = (1/L)1/2 exp(2pinx/L) and the energies En = 2 hbar2 p2 n2 / (mL2).

(b) What is the time dependence of Yn(x,t)?

(c) What values of n are allowed? What is the degeneracy of the state |n>?

(d) In state |n> of this system, what values of p are allowed, and what is the probability of a measurement of pop giving each of these values?

 

2. Suppose that in the preceding problem, a term H' = b d(x - L/2) with b small is added to the Hamiltonian. Calculate to first order in the parameter b the energy of the state(s) whose unperturbed energy is 2 hbar2 p2 / (mL2)

 

3. (a) An electron is in a state with spin up along the z-axis, i.e.

    1
    0  .
What is the probability of finding that electron in a state that is spin-up along the x-axis? Justify your answer.

    (b). If only electrons whose spin is up-along-x are kept in the apparatus after determining the spin direction, what is the wave function of the electron after the measurement?

    (c). What is the probability of now finding the electron in a state that has spin down along the z axis? Prove your answer.

For reference, the Pauli spin matrices for x, y, and z are

      0  1     0  -i     1   0
      1  0  ,  i   0  ,  0  -1
respectively.

 

4. Let us invent a particle called the nothun, which has spin 1/2, feels a Coulomb ( - e2 / 4 p e 0 r) attraction to a proton, and interacts with any other nothun with a potential aS1.S2 , where the parameter a is small. Two nothuns do not exert Coulomb forces on each other. The mass m of a nothun is small compared to the mass of a proton.

(a) Neglecting a, what is the properly symmetrized ground state of a system of 2 nothuns and a proton?

(b) What is the total spin S of the nothuns in this state?

(c) To first order in a, what is the energy of the ground state of this system?

 

5. (a) Show that y1(x) = [4 m w/ (p hbar)]1/4 x exp( - x2 / 2) where x = (m w / hbar)1/2 x is a solution for the one-dimensional harmonic oscillator with energy E = 3 h-bar w / 2 .

(b) Using the results of part (a), find the energy and wavefunction for the lowest state(s) in the three-dimensional harmonic oscillator with an angular momentum whose magnitude is h-bar (l=1). What is the degeneracy of this state?


PHYS 424 Final Exam

December 14, 2001

Ñ2 = (1/r2)/r (r2/r) + 1/(r2sinq) /q (sinq /q) + 1/(r2 sin2q) 2/f2

Y00 = 1/sqrt(4p)
Y10 = sqrt[3/(4p)] cos(q)
Y1-1 = + sqrt[3/(8p)] sin(q) e -if       Y11 = - sqrt[3/(8p)] sin(q) e +if

 

1. Consider the potential

V(x) = 0,         0 < x < a
¥ ,       x < 0 or x > a

(a) Show carefully that the states |n> = (2/a)1/2 sin(pnx/a) and the energies En = hbar2p2n2/a2.

(b) What is the time dependence of Yn(x,t)?

(c) What values of n are allowed? What is the degeneracy of the state |n>?

(d) Write down the matrix <n'|H|n> [at least enough of it that the form is apparent].

(e) In state |n> of this system, what values of p are allowed, and what is the probability of a measurement of pop giving each of these values?

 

2. If in the preceding problem, a term H' = b cos(2px/a) with b small is added to the Hamiltonian, what is the energy of each state to first order in the parameter b? [Hint: 2 sin A sin B = cos(A+B) - cos(A-B) and 2 cos A cos B = cos(A+B) + cos(A-B) ].

 

3. Given that the operators     S± = Sx ± iSy     obey     S±|s=1/2, sz=m>   =   hbar |s=1/2, sz=m±1>     whenever the state on the right-hand side of the relation exists, show that |s=1/2, sz=1/2> is an eigenstate of the operator S2 with eigenvalue (3/4)hbar2 .

4. For the Hamiltonian H = T + V = p2/(2m) + (1/2)mw2x2 use the operators a± = [1/sqrt(2m)] [px ± imwx] to show that <T> = <V> , where the expectation values are taken in an eigenstate of the Hamiltonian. [If you must refer to an integral or a matrix element that involves an integral to work this problem, name it and do not perform the integration. More credit will be awarded for a solution that does not need the specific value of any integral.]

 

5.Consider the potential

V(r) = 0,         0 < r < a
¥ ,       r > a
where r is the radial coordinate in spherical coordinates.

(a) Show that the l= 1 Y11 given in the box at the top of the exam gives the angular dependence of some of the states, and find the differential equation for the radial dependence of these l=1, ml=1 states.

(b) Without solving for the radial dependence find the best minimum value you can for the number of states degenerate with (having the same energy as) each one of these states.

(c) Is it guaranteed, likely, unlikely, or impossible that the actual degeneracy is higher than your minimum? Explain.