Help with commutator question please

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Homework Help Overview

The discussion revolves around deriving the commutator [H,P] in the context of quantum mechanics, where H is the Hamiltonian operator and P is the momentum operator. The original poster expresses confusion over obtaining a zero result and questions the conditions under which momentum remains a constant of motion, particularly in relation to the potential v(x).

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of the commutation relation and the expansion of the potential as a Taylor series. There are attempts to clarify the steps involved in deriving the commutator and questions about the treatment of terms within the commutator.

Discussion Status

Some participants have provided guidance on the linearity of the commutator and the implications of the Hamiltonian's structure. There is an ongoing exploration of the derivation process, with various interpretations and methods being discussed without a clear consensus on the resolution of the original poster's confusion.

Contextual Notes

Participants mention the use of h-bar and its normalization, as well as the need to clarify the treatment of addition within the commutator. There is an acknowledgment of the potential complexity of the problem despite it being described as elementary.

jus8727
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consider a general one dimensional potential v(x) drive an expression for the commutator [H,P] where h is hamiltonian operator and momentum operator. i keep getting zero and i don't think i should. since next part of homework question sais what condition must v(x) satisfy so that momentum will be constant of the motion recall that this is true if the momentum communtes with the hamiltonian. so i don't think it should zero. any help would be great trtying to do all homework problems to prepare for final!
 
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[tex][P^{2}/2m + V(x) , P] = [ V , P] = -i \frac{dV}{dx}[/tex]
 
thats how i started but didnt arrive at that can u show a little bit more detail if u don't mind.
thanks a lot though
 
Consider the action of the commutator on a wavefunction

[H, P] psi(x)

(so, we work in the position representation). Write out the commutator explicitely:

H P psi - P H psi
 
yes that's what I am doing but I am still getting zero
 
Expand the potential as a Taylor series and use the commutation relation [tex][x,p]=i \hbar[/tex].
 
samalkhaiat said:
[tex][P^{2}/2m + V(x) , P] = [ V , P] = -i \frac{dV}{dx}[/tex]

[tex][P^{2}/2m, P] + [V , P] = [V,P][/tex]

because [P,P] = 0.

then

[tex] [H,P] \phi(x) = [V(x) , id/dx] \phi(x) = iV \frac{d \phi}{dx} -i\frac{d}{dx} \{V(x)\phi(x)\} = \{-i dV/dx\} \phi(x)[/tex]
 
um is there an easier way? like the first respnse seems right but idk how to get there its an elementary problem that i have I am sure
 
samal where is the h bar term? is that a property of commutator i have never seen that before
 
  • #10
i think the problem is i don't know what to do when we have an additon in the commutator i don't know how to treat it
 
  • #11
The commutator is linear [A+B,C] = [A,C] + [B,C]. Just write it out and you'll see that.
 
  • #12
jus8727 said:
samal where is the h bar term? is that a property of commutator i have never seen that before

I always set my h bar equal to 1. you can put it back in the equation. The first point you need to know is

[A + B , C] = [A,C] + [B,C]

the second point, an (differential) operator in the commutator acts on all the stuff on the right, so

[tex][A , i\hbar d/dx] f(x) = A(i\hbar df(x)/dx) - i\hbar (d/dx)(Af(x))[/tex]
 
  • #13
oh got it thanks a lot guys!
 

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