Where Did I Go Wrong? Troubleshooting a Commutator Relation

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Homework Help Overview

The discussion revolves around a commutator relation involving the Dirac Hamiltonian and angular momentum operators in quantum mechanics. The original poster is attempting to derive the commutator [H_D, L_k] and is uncertain about a missing factor in their result.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster outlines their calculations step-by-step but questions where they might have gone wrong, particularly regarding the missing factor of -i in their result.
  • Some participants suggest that the inclusion of certain terms, like the beta m, may be unnecessary and that the angular momentum operator might be incorrectly defined.
  • Others raise concerns about notation and conventions used in the formulation of angular momentum, indicating potential sources of confusion in the calculations.

Discussion Status

Participants are actively engaging with the original poster's calculations, offering observations and alternative perspectives. There is a recognition of differing conventions in notation, and some participants are exploring the implications of these differences on the calculations. No explicit consensus has been reached, but several productive lines of inquiry are being pursued.

Contextual Notes

There are indications of confusion regarding the definitions and conventions used for angular momentum and the Hamiltonian, which may affect the calculations. The original poster is also grappling with the implications of these conventions on their results.

Spinny
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Hi, I've got a commutator relation I'm trying to figure out here. I don't know what I'm doing wrong, but I don't seem to be able to get it right, so hopefully someone can help me through it.

Anyway, here's the problem. We're given the Dirac Hamiltonian [tex]H_D = \alpha_j p_j + \beta m[/tex], where [tex]p_j = -i\nabla_j[/tex] and the angular momentum components [tex]L_k = i\epsilon_{kln}x_lp_n[/tex]. We are then going to show the commutator relation

[tex][H_D,L_k] = -i\epsilon_{kln}\alpha_lp_n[/tex]

Here's what I've got so far:

[tex][H_D,L,k]\psi = (H_DL_k-L_kH_D)\psi[/tex]

[tex]=(\alpha_j p_j+\beta m)i\epsilon_{kln}x_lp_n\psi -i\epsilon_{kln}x_lp_n(\alpha_jp_j+\beta m)\psi[/tex]

[tex]=\alpha_j p_j i\epsilon_{kln}x_lp_n\psi +\beta mi\epsilon_{kln}x_lp_n\psi -i\epsilon_{kln}x_lp_n\alpha_jp_j\psi-i\epsilon_{kln}x_lp_n\beta m\psi[/tex]

So far, (hopefully) so good. Now, as far as I can see, the second and the last part cancel, so we're left with

[tex][H_D,L_k]\psi = \alpha_j p_j i\epsilon_{kln}x_lp_n\psi - i\epsilon_{kln}x_lp_n\alpha_jp_j\psi[/tex]

Rewriting the first part we get

[tex]i\epsilon_{kln}p_n\alpha_j p_j(x_l\psi)[/tex]

and knowing that [tex]p_j[/tex] is a differential operator, we use the product rule, and get

[tex]i\epsilon_{kln}p_n(\psi \alpha_j p_j x_l + x_l\alpha_jp_j \psi)[/tex]

We then have that [tex]p_j x_l = -i[/tex] for j = l, and 0 for j != l. Thus

[tex]i\epsilon_{kln}p_n(-i\alpha_l\psi + x_l\alpha_jp_j\psi)= \epsilon_{kln}p_n\alpha_l \psi+i\epsilon_{kln}p_nx_l\alpha_jp_j\psi[/tex]

Putting this back in we get

[tex][H_D,L_k]\psi = \epsilon_{kln}p_n\alpha_l \psi+i\epsilon_{kln}p_nx_l\alpha_jp_j\psi- i\epsilon_{kln}x_lp_n\alpha_jp_j\psi[/tex]

But now the last two parts cancel, and we're left with

[tex][H_D,L_k]\psi = \epsilon_{kln}p_n\alpha_l \psi[/tex]

This is almost what I was supposed to get, only the factor -i is missing. It seems so close, so hopefully I'm not way off, but, where did I go wrong?!?
 
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One observation (not a solutoin to your problem, but i'll grt some paper for that in a second), is that you unnecessarily include the beta m in you calcs.

if H=a_jp_j+bm, then commutating anything with H is the same as commutating it with just a_jp_j since bm is a constant and commutes with everything (it is a central element).

you also don't need to include the phi either.

just in case you want to write this out in latex again you can save yourself some bother.
 
I think you have you angular momentum operator slightly wrong (i'm not an expert here) but it ought to be

[tex]L_k =-i\epsilon_{lkn}x_k\partial_n[/tex]

this changes everything in your post by a factor if -i as required I think, though I've not gotten down to checking the signs with any great enthusiasm. (i'm a pure mathematician, and so if it's true up to minus signs [we call this mod 2] then it's true full stop.)
 
matt grime said:
I think you have you angular momentum operator slightly wrong (i'm not an expert here) but it ought to be

[tex]L_k =-i\epsilon_{lkn}x_k\partial_n[/tex]

this changes everything in your post by a factor if -i as required I think, though I've not gotten down to checking the signs with any great enthusiasm. (i'm a pure mathematician, and so if it's true up to minus signs [we call this mod 2] then it's true full stop.)

Thanks for your insight. I'm not able to see, however, how it is the ang. mom. that's incorrect. The -i still comes from the mom. in the hamiltonian and cancel the i in the ang. mom.

Anyway, I'm still having trouble finding out where that ang. mom. actually came from, I haven't been able to find a similar anywhere yet (at least not one I recognize as the one given in this problem). If I ever get in the mood again, I'll review the problem with your insight in mind.
 
Spinny said:
Thanks for your insight. I'm not able to see, however, how it is the ang. mom. that's incorrect. The -i still comes from the mom. in the hamiltonian and cancel the i in the ang. mom.

Anyway, I'm still having trouble finding out where that ang. mom. actually came from, I haven't been able to find a similar anywhere yet (at least not one I recognize as the one given in this problem). If I ever get in the mood again, I'll review the problem with your insight in mind.
The angular momentm components are incorrectly written. They should either be written without the "i" (when writing in terms of momentum components) or as Matt says (on plugging in for the mom. components).

Also note that the non-rel KE term is written using Einstein notation, so it really is the sum of all three products (ie : [itex]\sum_{j=k,l,n} \alpha _j p_j[/itex] ).
 
Spinny said:
Thanks for your insight. I'm not able to see, however, how it is the ang. mom. that's incorrect. The -i still comes from the mom. in the hamiltonian and cancel the i in the ang. mom.

Anyway, I'm still having trouble finding out where that ang. mom. actually came from, I haven't been able to find a similar anywhere yet (at least not one I recognize as the one given in this problem). If I ever get in the mood again, I'll review the problem with your insight in mind.


The problem is that you're mixing notations. Angular momentum can be with or without the i, but that changes it from a nabla to a p or back again. So, you're using one convention in your working out but the solution is written with the other convention, that is why they don't agree. At least, that is my analysis: i checked this relation and that seems to be the problem.
 

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