Quantum Mechanical Harmonic Oscillator Problem Variation

In summary, at time t < 0 there is an infinite potential for x<0 and for x>0 the potential is 1/2m*w^2*x^2 (harmonic oscillator potential. Then at time t = 0 the potential is 1/2*m*w^2*x^2 for all x.The particle is in the ground state.Assume t = 0+ = 0-The probability that a measurement will give the value hbar*w/2 is 1/(2*∏).The probability that a measurement will give the value 3*hbar*w/2 is 1/4.
  • #1
jcharles513
22
0

Homework Statement


At time t < 0 there is an infinite potential for x<0 and for x>0 the potential is 1/2m*w^2*x^2 (harmonic oscillator potential. Then at time t = 0 the potential is 1/2*m*w^2*x^2 for all x.
The particle is in the ground state.
Assume t = 0+ = 0-
a) what is the probability that a measurement will give the value hbar*w/2?
b) what is the probability that a measurement will give the value 3*hbar*w/2?

Homework Equations


This seems more conceptual than anything. The eigenenergies for the harmonic oscillator might help \hbar*ω(n+1/2)

The Attempt at a Solution



I know that at t <0 the half harmonic oscillator only allows the odd eigenfunctions to survive and then when the infinite potential is removed and a full harmonic oscillator exists for t>0 all of the eigenfunctions can exist but I don't know how to get probability from this knowledge.

I apologize for my lack of latex. I couldn't find an hbar in the latex reference and didn't know how to do it on my own.
 
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  • #2
Suppose you had mathematical expressions for the following:

1. The wavefunction ##\psi(x)## at time t = 0 for -∞< x ∞

2. The eigenfunctions ##\phi_0(x)## and ##\phi_1(x)##of the full harmonic well corresponding to ##E = \hbar ω/2## and ##E = 3\hbar ω/2##, respectively.

How would you use these functions to determine the probabilities asked for?

If you need some help, see page 2 of http://www.umich.edu/~gevalab/Geva/lecture/chem461/Chapter3.pdf
 
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  • #3
If I was given the wavefunction ψ(x). The probability is just calculated <[itex]\phi_0[/itex]|ψ(x)>.

For t > 0, Ʃ<[itex]\phi_n[/itex]|ψ(x)>|ψ(x)> will be the expanded wavefunction. This means that to get the different values I would just integrate and multiply by the [itex]\phi_n^*[/itex] to get the probabilities where n = 0,1.
 
  • #4
jcharles513 said:
If I was given the wavefunction ψ(x). The probability is just calculated <[itex]\phi_0[/itex]|ψ(x)>.

For t > 0, Ʃ<[itex]\phi_n[/itex]|ψ(x)>|ψ(x)> will be the expanded wavefunction. This means that to get the different values I would just integrate and multiply by the [itex]\phi_n^*[/itex] to get the probabilities where n = 0,1.

Good. But keep in mind that <[itex]\phi_0[/itex]|ψ(x)> is the "probability amplitude" rather than the probability (and the functions need to be normalized).
 
  • #5
TSny said:
Good. But keep in mind that <[itex]\phi_0[/itex]|ψ(x)> is the "probability amplitude" rather than the probability (and the functions need to be normalized).

If that's the probability amplitude than the probability would just be the magnitude of that squared correct? So now all I need is to figure out the form of the wave function before and after.

t < 0 the wave function is in the groundstate of the half harmonic oscillator so for x >0 it looks like the 1st excited state of the full harmonic oscillator and for x < 0, it goes to 0.

Then when it's switched on it's the full harmonic oscillator but I'm not sure what eigenstates make up the wave function is it just the ground state 1st and 2nd excited state?
 
  • #6
Yes. That all sounds good. You'll need to look up the wavefunctions for the eigenstates of the full harmonic oscillator potential that correspond to the ground state and the first excited state. You won't need the 2nd excited state.
 
  • #7
I got the probability for hbarω/2 = 1/(2*∏) and then 3hbarω/2 = 1/4. What did you get?
 
  • #8
I haven't worked out the integrals. Maybe I will if I get a chance.

Off hand, though, the answer for 3hbarω/2 doesn't look right to me. Did you normalize the initial wave function properly?
 
  • #9
I believe so. The normalized initial wavefunction is just A_0*(1/√2)*2*x'*exp(-x'^2/2) where x' = (xmω/hbar)^(1/4) and A_0 = (1/∏)^(1/4). Am I missing something?
 
  • #10
Remember, that the initial wave function is zero for negative x. So, you need to choose the nomalization factor with that in mind.
 
  • #11
Ah yes of course. So that means I would have a √2 out front for the normalization. So I would multiply each of my probabilities by two. I get 1/∏ for the ground state and 1/2 for the first excited state for t > 0.
 
  • #12
Good. That's what I get, too.
 
  • #13
Good. Thanks for your help.
 

1. What is a quantum mechanical harmonic oscillator problem?

A quantum mechanical harmonic oscillator is a theoretical model used to describe the behavior of particles at the quantum level. It is a system that consists of a particle moving back and forth between two points, with a restoring force that is proportional to the displacement from the equilibrium position. It is an important concept in quantum mechanics and has applications in various fields such as chemistry, physics, and engineering.

2. What is the variation of the quantum mechanical harmonic oscillator problem?

The variation of the quantum mechanical harmonic oscillator problem refers to the different ways in which the problem can be solved or analyzed. This includes variations in the potential energy function, boundary conditions, and the type of oscillator (e.g. one-dimensional, two-dimensional, etc.). Different variations can lead to different solutions and insights into the behavior of the system.

3. What is the significance of the quantum mechanical harmonic oscillator problem?

The quantum mechanical harmonic oscillator problem is significant because it is one of the few quantum mechanical problems that can be solved exactly. This means that the behavior of the system can be predicted with high accuracy, making it a valuable tool in understanding the quantum world. It also serves as a model for more complex systems and has applications in fields such as quantum optics, quantum computing, and nanotechnology.

4. How is the quantum mechanical harmonic oscillator problem solved?

The quantum mechanical harmonic oscillator problem is typically solved using mathematical techniques such as the Schrödinger equation, perturbation theory, and the variational method. These methods allow us to calculate the energy levels, wave functions, and other properties of the system. In some cases, the problem can also be solved using numerical methods such as matrix diagonalization.

5. What are some real-world examples of the quantum mechanical harmonic oscillator problem?

The quantum mechanical harmonic oscillator problem has many real-world applications. For example, it is used to describe the behavior of electrons in atoms, the vibrations of molecules, and the motion of particles in a crystal lattice. It is also relevant in fields such as quantum optics, where it is used to describe the behavior of photons in optical cavities, and in quantum computing, where it is used to model the behavior of qubits.

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