Raising and lowering operators & commutation

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Homework Help Overview

The discussion revolves around the commutation relation of raising and lowering operators in quantum mechanics, specifically showing that [a+, a-] = -1. The operators are defined in terms of position (X) and momentum (P) operators, with participants exploring the implications of their definitions and the resulting calculations.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants attempt to compute the commutation relation [a+, a-] by substituting definitions of the operators and simplifying the expressions. Questions arise regarding the order of operations and the role of test functions in the calculations. Some participants express confusion over why their results yield zero and question the assumptions made about operator commutation.

Discussion Status

The discussion is ongoing, with participants providing insights into the nature of operator commutation and the importance of careful manipulation of operators. Some guidance has been offered regarding the use of test functions and the canonical commutation relation, but a clear resolution has not yet been reached.

Contextual Notes

Participants note the challenge of working with operators that do not commute and the necessity of including test functions in calculations. There is also mention of specific constants and factors that may influence the final results, indicating potential constraints in the problem setup.

Werbel22
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Homework Statement



Show [a+,a-] = -1,

Where a+ = 1/((2)^0.5)(X-iP)
and a- = 1/((2)^0.5)(X+iP)

and

X = ((mw/hbar)^0.5)x

P = (-i(hbar/mw)^0.5)(d/dx)2. The attempt at a solution

It would take forever to write it all up, but in summary:

I said:

[a+,a-] = (a+a- - a-a+)

then subbed in equations to finally get:

-((hbar/mw)^0.5)(d/dx)((mw/hbar)^0.5)x +((hbar/mw)^0.5)(d/dx)((mw/hbar)^0.5)xwhich cancels out to zero, I don't get why! I made sure I did them in the right order, is there something I'm missing? Is it not just a matter of subbing these formulae in?

I put lambda as the wavefunction in when I was doing it on paper, so that the (d/dx) had something to operate on, but it didn't seem to help as it still gives zero.

Please help, I'm really stuck as to what to do :(
 
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Ignoring the constant factors you'll have something like have
[a+,a-] = [x - ip, x+ip] = [x,x] + [x,ip] - i[p,x] + [p,p] = i[x,p] - i[p,x] = 2i[x,p]

Now what is [x,p] ?
 
[X,P] = xp - px ?

When I sub in the equations for those now, I get zero for [x,p], which gives zero for [a+,a-].

I got down to:

[x,p] = (-i(d/dx)(x)) - (-i(d/dx))x
= -i + i = 0

:S I don't get why I can't get the answer.
 
Also, how did you compute [a+,a-]? Remember, operators do not normally commute, so you must be careful about what you switch around. Also, you typically can't determine a commutation rule without having a "test function" for your operators to act on. d/dx makes no sense by itself unless it acts on something for example.
 
Yeah, but I thought in the example d/dx was operating on x, just to give 1. When I put it in, in my original post, it didn't make a difference.

I know operators don't commute, but when I sub IN the actual operator (say into xp - px) it isn't an operator anymore, it's just some variables/constants, so I have just numbers and don't get how THEY can't commute :S
 
You really need to be more careful with this.
Consider xp operating on f(x). This is x * -ih d/dx f(x) = -ih x * f ' (x)
Now consider px operating on f(x). This is -ih * d/dx (x f(x)) = -ih (f(x) + x*f '(x)) (by the product rule)
 
I'm still stuck. I understand that last post, and it has helped.

But regardless if I take that into account, I don't see how having a f'(x) helps me, I tried doing it that way, and seeing I end up with a combination of f(x) and f'(x) in my final answer I don't see how that will give 1 :(
 
Well if you understand the last post, you should be able to calculate [x,p]. The "f" is a test function, and should not be included in the final commutator.

[x,p]\psi = xp\psi - px\psi
[x,p]\psi = -i\hbar x\psi'(x) - ( -i\hbar x\Psi'(x) -i\hbar\psi(x))
[x,p]\psi = i\hbar\psi(x)

Which means that, after "factoring out" the test function,
[x,p] = i\hbar
This is known as the canonical commutation relation, and is one of the most important equations in quantum mechanics, if not the most. Don't forget it!

Now remember in the first post I showed that
<br /> [a^+, a^-] \sim [x, p]
up to some constant. I hope you'll be able to see why getting 1 as the answer is plausible.
 

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