Harmonic Oscillator Analytical Mechanics: Creation/Annihilation Ops

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Homework Help Overview

The discussion revolves around the Hamiltonian for a one-dimensional harmonic oscillator, specifically focusing on expressing it in terms of creation and annihilation operators. Participants are exploring the implications of these expressions and the associated Poisson brackets, as well as the equations of motion for the operators.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants attempt to express the Hamiltonian in terms of the operators a and a*. There are questions regarding the definitions of conjugate momentum and coordinates, as well as the meaning of "equations of motion." Some participants suggest starting with the time-derivative of the operators.

Discussion Status

There are multiple interpretations being explored regarding the algebra involved in part (a) and the treatment of a and a* as either operators or coordinates. Some participants have provided guidance on how to approach the equations of motion, while others have expressed uncertainty about the algebraic manipulations and the implications of the quantum harmonic oscillator.

Contextual Notes

Participants note potential confusion stemming from the treatment of a and a* and their relationship to quantum mechanics, as well as the implications of the vacuum energy term in the Hamiltonian. There is also mention of homework constraints and the need for clarity in definitions and expressions used in the problem.

Loxias
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Homework Statement


The Hamiltonian for the one-dimensional harmonic oscillator is given by:
[tex]H = \frac{p^2}{2m}+ \frac{mw^2q^2}{2}[/tex]

Homework Equations



(a) Express H in terms of the following coordinates:

[tex]a = \sqrt{\frac{mw}{2}} (q+i\frac{p}{mw})[/tex]
[tex]a^* = \sqrt{\frac{mw}{2}} (q-i\frac{p}{mw})[/tex]

(b) Calculate the following Poisson Brackets: {a*,H} {a,H}, {a, a*}
(c) Write and solve the equations of motion for a and a.

The Attempt at a Solution



a. simple algebra :
[tex]H = waa^*[/tex]

b. again, algebra :
[tex]\{a^*,H\} = iwa^*, \{a,H\} = -iwa, \{a,a^*\} = -i[/tex]

c.

this is where I'm having trouble. I don't really get the question.. what's the conjugate momentum? what's the coordinates? where do I start from? :)

Thanks
 
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Loxias said:
(c) Write and solve the equations of motion for a and a. [my edit--I assume you mean a and a*?]

...
c.

this is where I'm having trouble. I don't really get the question.. what's the conjugate momentum? what's the coordinates? where do I start from? :)

Thanks

Perhaps you should start with, 'what does it mean "equations of motion"?' This means, in Hamiltonian dynamics, that you need to find the time-derivative of a and a-star.
 


Also, I think part a is wrong. You may want to double check your algebra.
 


I rechecked part a again, and also solved it using another method, got the same answer. I also think It's right since it resembles the quantum hamiltonian, without [tex]\hbar[/tex] and [tex]\frac{1}{2}[/tex], which makes sense.

For the third part, I used [tex]\dot{a} = \{a,h\}[/tex] and solved it.
Before I did that simple thing, I expressed q and p using a, a*, wrote an expression for [tex]\dot{a}, \dot{a^*}[/tex] and then used the hamiltonian equations of motion to express [tex]\dot{p}, \dot{q}[/tex] using a, a*, and got the same result :)

Thanks for your help :smile:
 


Loxias said:
I rechecked part a again, and also solved it using another method, got the same answer. I also think It's right since it resembles the quantum hamiltonian, without [tex]\hbar[/tex] and [tex]\frac{1}{2}[/tex], which makes sense.

The way I see it, it pretty much is the quantum harmonic oscillator with [itex]\hbar=1[/itex] units:

[tex] q^2=\frac{1}{2m\omega}\left(a+a^*\right)^2[/tex]

[tex] p^2=-\frac{m\omega^2}{4}\left(a-a^*\right)^2[/tex]

so that

[tex] \begin{array}{ll}<br /> H&=\frac{p^2}{2m}+\frac{m\omega^2q^2}{2} \\ <br /> &=-\frac{\omega}{4}\left(aa-aa^*-a^*a+a^a^*\right)+\frac{\omega}{4}\left(aa+aa^*+a^*a+a^*a^*\right) \\<br /> &=\frac{\omega}{4}\left(2aa^*+2a^*a\right) \\<br /> &=\omega\left(aa^*+\frac{1}{2}\right)<br /> \end{array}[/tex]

It looks, though, that the factor of [itex]\frac{1}{2}[/itex] isn't necessary for parts (b) and (c), just part (a)--this is because you can solve the Poisson brackets in terms of [itex]q[/itex] and [itex]p[/itex], in which case you can use the Hamiltonian you began with.
 
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I think you are treating a, a* as operators (used commuting relation in the last part, if I'm not mistaken), while here they are simply coordinates, and aa* = a*a.
Please note that you expressed [tex]p^2, q^2[/tex] in a wrong way but then corrected it in H.

Also, my algebra is

[tex]waa^* = \frac{mw^2}{2} (q^2 + \frac{p^2}{(mw)^2}) = \frac{p^2}{2m} + \frac{mw^2q^2}{2} = H[/tex]

I also did this by expressing q and p using a, a* and got the same result.
 


Loxias said:
I think you are treating a, a* as operators (used commuting relation in the last part, if I'm not mistaken),

Ha, that I am. I have been stuck on my QM for the last several days before my final on Wednesday--of course it doesn't help that your title says "creation/annihilation ops". Your answer is right then.
Loxias said:
Please note that you expressed [tex]p^2, q^2[/tex] in a wrong way but then corrected it in H.

Right, there should have been a squared term on the parenthesis--just fixed those too. Glad I could help!
 


If I remember correctly, the half in the quantum hamiltonian is the vacuum energy, and is a quantum effect, not classical. (This all may be wrong, don't take me up for it :) )
 


Good luck on your exam!
 
  • #10


Loxias said:
Good luck on your exam!

Thanks!
 

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