Solve Taylor Series & Groups Homework: Show T(a) = exp(iap_x)

  • Thread starter Thread starter limddavid
  • Start date Start date
  • Tags Tags
    Taylor
limddavid
Messages
6
Reaction score
0

Homework Statement



A translation operator T(a) coverts ψ(x) to ψ(x+a),

T(a)ψ(x) = ψ(x+a)

In terms of the (quantum mechanical) linear momentum operator p_x = -id/dx, show that T(a) = exp(iap_x), that is, p_x is the generator of translations. Hint. Expand ψ(x+a) as a Taylor series.

Homework Equations



Groups?

The Attempt at a Solution



I'm lost at the hint. To expand ψ(x+a) as a Taylor series, don't I need a point around which to expand it?
 
Physics news on Phys.org
limddavid said:

Homework Statement



A translation operator T(a) coverts ψ(x) to ψ(x+a),

T(a)ψ(x) = ψ(x+a)

In terms of the (quantum mechanical) linear momentum operator p_x = -id/dx, show that T(a) = exp(iap_x), that is, p_x is the generator of translations. Hint. Expand ψ(x+a) as a Taylor series.

Homework Equations



Groups?

The Attempt at a Solution



I'm lost at the hint. To expand ψ(x+a) as a Taylor series, don't I need a point around which to expand it?

Yes- a.
 
Ok. so would the taylor series be:

ψ(a+a)+ψ'(a+a)(x-a)+ψ''(a+a)*(x-a)^2/2!+... ? and maybe disregard the higher order terms O(3)? Or would it be

ψ(a)+ψ'(a)*(x)+ψ''(a)*(x)^2/2!+... ? Either way, I'm not sure how I would prove that T(a) is the given exponential function..
 
You want to expand about x=x, i.e., ψ(x+a) = ψ(x)+...
 
ok.. so i expanded that, and got ψ(x)+aψ'(x)+a^2*ψ''(x)/2!+ ...

But the LHS gives me:

e^(i*a*px)[ψ(x)]=e^(a*dψ/dx)=e^(-iak*ψ(x)), which is clearly not the left hand side. Am I interpreting the operator px wrong? This class is not a quantum dynamics class, so I'm having difficulty figuring out what I'm missing.
 
You can't pull ψ(x) into the exponent like that because ψ(x) isn't an eigenfunction of the operator \hat{p}_x.

It's not be exactly obvious what the expression e^{ia\hat{p}_x} means. How do you exponentiate an operator? The answer is that it's defined by the Taylor series for ex:
e^{ia\hat{p}_x} \equiv 1+ia\hat{p}_x+\frac{(ia\hat{p}_x)^2}{2!}+\cdotsWhat do you get when you apply the righthand side to ψ(x)?
 
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top