Prove Commutator Identity: e^xA B e-xA = B + [A,B]x + ...

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SUMMARY

The discussion centers on proving the commutator identity: e^{x \hat A} \hat B e^{-x \hat A} = \hat B + [\hat A, \hat B]x + \frac{[\hat A, [\hat A, \hat B]]x^2}{2!} + \frac{[\hat A, [\hat A, [\hat A, \hat B]]]x^3}{3!} + ... The participants analyze the series expansions of the exponential functions and the implications of rearranging commutation orders. The key takeaway is that proper multiplication and collection of terms in powers of x lead to the desired result, emphasizing the importance of understanding operator algebra and commutation relations.

PREREQUISITES
  • Understanding of operator algebra and commutation relations
  • Familiarity with Taylor series expansions for e^{x} and e^{-x}
  • Knowledge of the properties of linear operators in quantum mechanics
  • Experience with manipulating series and power expansions
NEXT STEPS
  • Study the derivation of the Baker-Campbell-Hausdorff formula
  • Learn about the implications of the Lie algebra structure in quantum mechanics
  • Explore advanced topics in operator theory and their applications
  • Investigate the role of commutators in quantum mechanics and their physical significance
USEFUL FOR

Quantum mechanics students, physicists, and mathematicians interested in operator theory and commutation relations will benefit from this discussion.

kreil
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Homework Statement




Prove the following identity:

e^{x \hat A} \hat B e^{-x \hat A} = \hat B + [\hat A, \hat B]x + \frac{[\hat A, [\hat A, \hat B]]x^2}{2!}+\frac{[\hat A,[\hat A, [\hat A, \hat B]]]x^3}{3!}+...

where A and B are operators and x is some parameter.

Homework Equations


e^x = 1+x+\frac{x^2}{2!}+\frac{x^3}{3!}+...
e^{-x} = 1-x+\frac{x^2}{2!}-\frac{x^3}{3!}+...

The Attempt at a Solution



\hat B e^{-x \hat A} = \hat B - [\hat B, \hat A]x + \frac{[[\hat B, \hat A], \hat A] x^2}{2!}+...

It seems after I rearrange the commutation orders, the signs all become positive and this is the required result, so I know I must be doing something wrong. I think it has to do with how I'm multiplying out B into the series..

i.e. \hat B (\hat A x)^2 = [\hat B, \hat A \hat A] x^2...??

or \hat B (\hat A x)^2 = [[\hat B, \hat A], \hat A] x^2...??
 
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kreil said:
It seems after I rearrange the commutation orders, the signs all become positive and this is the required result, so I know I must be doing something wrong. I think it has to do with how I'm multiplying out B into the series..

i.e. \hat B (\hat A x)^2 = [\hat B, \hat A \hat A] x^2...??

or \hat B (\hat A x)^2 = [[\hat B, \hat A], \hat A] x^2...??

Neither is correct.

\hat{B}(x\hat{A})^2=BA^2x^2[/itex]<br /> <br /> You won&#039;t have anything involving commutators until you multiply by both exponentials and collect terms in powers of the parameter x.
 
ahh I see it now I think..

e^{x \hat A} \hat B e^{-x \hat A} = \left ( 1+\hat A x + \frac{1}{2} \hat A^2 x^2 + \frac{1}{6} \hat A^3 x^3+... \right ) \left ( \hat B - \hat B \hat A x + \frac{1}{2} \hat B \hat A^2 x^2 - \frac{1}{6}\hat B \hat A^3 x^3+... \right )

So I multiply this out, collect terms in powers of x, and simplify to the commutator relations

Thanks
 

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