Ladder operators and matrix elements...

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Discussion Overview

The discussion revolves around the calculation of matrix elements using ladder operators in quantum mechanics, specifically focusing on the expressions involving the momentum and position operators. Participants explore the implications of different states represented by "u" and how these affect the calculations.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • One participant requests help with calculating matrix elements and , questioning if the result is zero when "u" differs on both sides.
  • Another participant seeks clarification on the definitions of the operators P and X, and the meaning of "u".
  • Several participants discuss the representation of position and momentum operators in terms of ladder operators, providing formulas and rules for their application.
  • One participant explains how to compute the matrix element using the ladder operator rules, indicating that certain terms will yield zero due to orthogonality.
  • Another participant expresses confusion about how to handle multiple ladder operators in a product and how they interact with the states.
  • There is a suggestion that the thread should be moved to the Advanced Physics Homework section for better categorization.

Areas of Agreement / Disagreement

Participants generally agree on the use of ladder operators and the rules for their application, but there is uncertainty regarding the specific calculations and interpretations of the results, particularly concerning when terms equal zero.

Contextual Notes

Some participants express limitations in their background knowledge, particularly in physics, which may affect their understanding of the mathematical operations and concepts discussed.

Who May Find This Useful

Readers interested in quantum mechanics, particularly those studying ladder operators and matrix elements in the context of quantum states and operators.

Activeuser
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Please I need your help in such problems..
in terms of ladder operators to simplify the calculation of matrix elements... calculate those
i) <u+2|P2|u>
ii) <u+1| X3|u>
If u is different in both sides, then the value is 0? is it right it is 0 fir both i and ii?
when exactly equals 0, please explain slowly, my background is chemistry and not physics..
Thank you.
 
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You'll need to supply a bit more context...

I guess P and X are momentum and position operators respectively? But what is your "u"?
 
Well, in terms of ladder operators, X= (h/2mw)1/2(a+a+) you can say = constant (a+a+) it is a real
P=i(hwm/2)1/2 (a-a+) or constant (a-a+)
about u and u+1 are functions; some books write them like this and others write PSI or PHI of subscript u and u+1;I couldn't type that way as there is no symbols here.
a+a=n occupation number operator , [a,a+]=1

If needed I can give an example I know..
 
Activeuser said:
Well, in terms of ladder operators, X= (h/2mw)1/2(a+a+) you can say = constant (a+a+) it is a real
P=i(hwm/2)1/2 (a-a+) or constant (a-a+)
about u and u+1 are functions; some books write them like this and others write PSI or PHI of subscript u and u+1;I couldn't type that way as there is no symbols here.
a+a=n occupation number operator , [a,a+]=1

If needed I can give an example I know..

I'm assuming that |u\rangle means the state such that the number operator N = a^\dagger a has value u? In that case, it's completely straight-forward, if tedious, to compute expressions such as

\langle u+2 | P^2 | u \rangle

Just write P in terms of a and a^\dagger, and apply the rules:

a |u\rangle = \sqrt{u} |u - 1\rangle
a^\dagger |u\rangle = \sqrt{u+1} |u+1\rangle
\langle n | m \rangle = 0 if n \neq m
\langle n | n \rangle = 1

So P^2 = A (a^2 - a a^\dagger - a^\dagger a + (a^\dagger)^2) (for some constant A)
P^2 | u \rangle = A (a^2 |u \rangle - a a^\dagger |u\rangle - a^\dagger a |u\rangle + (a^\dagger)^2 |u\rangle)

Then you just work out what a^2 |u\rangle is, etc.
 
ok great. I know till this step, my question is to separate these operations and get the final out put like this
<u+2|aa|u> - <u+2|aa+|u> - <u+1|a+a|u>... so on
and solve each one on its own, when I get any different matrix output, the term equals 0; like <u+1|u> or <u+2|u-1>... right? Cuz my confusion is about this part.

the other part is how to work a3,, if aaa, the 1st one from left operates with the left , and the 1st a from right operates with the right function of the matrix, the middle a operator works with which function.. as it gives different values..
I am sorry for my silly questions, because this what I miss and can not find in books; it seems like a bases that I do not have.
 
Well, just look at the term

\langle u+2|a\ a|u \rangle

Use the rule: a |u\rangle = \sqrt{u} |u - 1\rangle. So that term simplifies(?) to:

\langle u+2|a\ a|u \rangle = \sqrt{u} \langle u + 2 | a | u-1\rangle

Use the same rule again: a |u-1\rangle = \sqrt{u-1} |u - 2\rangle. So we have:

\langle u+2|a\ a|u \rangle = \sqrt{u(u-1)}| \langle u + 2 | u-2\rangle

which is zero.

The only term you're going to get a nonzero result for is:

\langle u+2|a^\dagger\ a^\dagger|u \rangle
 
By the way, this should probably be in the Advanced Physics Homework section.
 
Thank you so much for this clarification.. it is very helpful.
Next time I will follow the right section.. new here.:smile:
 

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