Special Cases of the BCH Identity

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SUMMARY

The discussion centers on the application of the Baker-Campbell-Hausdorff (BCH) identity in quantum mechanics, specifically regarding Position (P) and Momentum (X) operators. The user initially attempts to express the product of exponentials involving these operators in the form of the BCH identity, leading to a conclusion that includes an additional term O'. The community emphasizes the need for a rigorous proof by starting from the left-hand side and demonstrating equality to the right-hand side, rather than assuming the form of O'. The user ultimately resolves the problem with guidance from forum members.

PREREQUISITES
  • Understanding of quantum mechanics, specifically Position and Momentum operators.
  • Familiarity with the Baker-Campbell-Hausdorff identity.
  • Knowledge of eigenvalues in quantum systems.
  • Basic algebraic manipulation skills in the context of operator equations.
NEXT STEPS
  • Study the derivation and applications of the Baker-Campbell-Hausdorff identity in quantum mechanics.
  • Explore the implications of non-commuting operators in quantum theory.
  • Learn about the significance of eigenvalues and eigenstates in quantum mechanics.
  • Practice proving identities involving operator exponentials through algebraic manipulation.
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Students and professionals in quantum mechanics, physicists working with operator algebra, and anyone seeking to deepen their understanding of the BCH identity and its applications in quantum systems.

WWCY
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Homework Statement


Hi all, I'm having trouble working on the following problem. Any assistance will be greatly appreciated.

Screen Shot 2018-09-16 at 11.54.42 PM.png
Here, the capital letters stand for Position and Momentum operators while the ##x', p'## stand for eigenvalues.

Homework Equations

The Attempt at a Solution



a) and b)

It seems that a) and b) can be written in the form of
$$e^{\frac{i}{\hbar}x'P}e^{\frac{i}{\hbar}p'X}$$
which I can then express in the form of the BCH identity
$$e^{\frac{i}{\hbar}x'P}e^{\frac{i}{\hbar}p'X} = e^{\frac{i}{\hbar}x'P + \frac{i}{\hbar}p'X + \frac{i}{2\hbar}x'p' + 0 + O'}$$
where I denote the other terms by ##O'##. If ##O' = 0##, I obtain b), if ##O' = \frac{i}{2\hbar}x'p' ##, I get a). Is this what the question was getting at? It does seem too convenient.

c)

I'm not too sure where to start with this one.

Thanks in advance for any help!
 

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WWCY said:

Homework Statement


Hi all, I'm having trouble working on the following problem. Any assistance will be greatly appreciated.

View attachment 230761Here, the capital letters stand for Position and Momentum operators while the ##x', p'## stand for eigenvalues.

Homework Equations

The Attempt at a Solution



a) and b)

It seems that a) and b) can be written in the form of
$$e^{\frac{i}{\hbar}x'P}e^{\frac{i}{\hbar}p'X}$$
which I can then express in the form of the BCH identity
$$e^{\frac{i}{\hbar}x'P}e^{\frac{i}{\hbar}p'X} = e^{\frac{i}{\hbar}x'P + \frac{i}{\hbar}p'X + \frac{i}{2\hbar}x'p' + 0 + O'}$$
where I denote the other terms by ##O'##. If ##O' = 0##, I obtain b), if ##O' = \frac{i}{2\hbar}x'p' ##, I get a). Is this what the question was getting at? It does seem too convenient.
It is not the best terminology to say that you express something "in the form of the BCH identity". People don't usually put it this way. What you have to do is to prove in each case that the left hand side is equal to the rhs, and the BCH identity can help you demonstrate this. So you should start from the expression on one side and end up on the expression on the other side, using any identity or algebraic manipulation you can do.

Focus on (a). Start from the left side and show that you get to the right side. This is almost what you did, but you did not complete your proof. You wrote

$$e^{\frac{i}{\hbar}x'P}e^{\frac{i}{\hbar}p'X} = e^{\frac{i}{\hbar}x'P + \frac{i}{\hbar}p'X + \frac{i}{2\hbar}x'p' + 0 + O'}$$

Now you must determine ##O'##. You cannot assume or choose the form it has. It has a unique expression and you must determine it. Once you will have shown what ##O'## is in this expression, you will have proven (a). Then we can discuss (b).
 
Hi @nrqed , I have actually managed to work out the problem, many thanks for your pointers!
 

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