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

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SUMMARY

The discussion focuses on proving that the translation operator T(a) in quantum mechanics can be expressed as T(a) = exp(iap_x), where p_x is the linear momentum operator defined as p_x = -i(d/dx). Participants explore the Taylor series expansion of the wave function ψ(x+a) around the point x, leading to the conclusion that p_x serves as the generator of translations. The correct application of the Taylor series and the interpretation of the operator exponentiation are crucial for understanding this relationship.

PREREQUISITES
  • Understanding of quantum mechanics, specifically linear momentum operators.
  • Familiarity with Taylor series expansions in mathematical analysis.
  • Knowledge of operator algebra and exponentiation in quantum mechanics.
  • Basic principles of wave functions and their transformations.
NEXT STEPS
  • Study the properties of the linear momentum operator p_x in quantum mechanics.
  • Learn about Taylor series and their applications in physics, particularly in quantum mechanics.
  • Research operator exponentiation and its significance in quantum theory.
  • Explore the concept of translation operators and their role in quantum mechanics.
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Students of quantum mechanics, physicists interested in operator theory, and anyone studying the mathematical foundations of quantum mechanics will benefit from this discussion.

limddavid
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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?
 
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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)?
 

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