Exponential of creation/annihilation operators

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The discussion centers on the exponential of creation and annihilation operators, specifically the equation e^{\phi^* a } f(a^{\dagger} , a ) = f(a^{\dagger} + \phi^*, a) e^{\phi^* a }. The participants highlight a derivation method using Taylor series and the commutation relation [a, g(a^\dagger)] ~=~ \frac{\partial g(a^\dagger)}{\partial a^\dagger}. This approach involves proving the relation by induction, starting with simple functions and extending to well-behaved analytic functions. The context is rooted in quantum field theory, particularly in the coherent state path integral formulation.

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  • Familiarity with creation and annihilation operators
  • Knowledge of Taylor series expansion
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  • Study the derivation of coherent state path integrals in quantum field theory
  • Learn about the implications of the commutation relation [a, g(a^\dagger)]
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ansgar
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Hello!

I found on this webpage:

http://www-thphys.physics.ox.ac.uk/people/JohnCardy/qft/costate.pdf

page 1, on the bottom

that

e^{\phi^* a } f(a^{\dagger} , a ) = f(a^{\dagger} + \phi^*, a) e^{\phi^* a }

I have tried to prove this, writing both as taylor series, but the problem is to understand the "hint" :(
 
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ansgar said:
I found on this webpage:

http://www-thphys.physics.ox.ac.uk/people/JohnCardy/qft/costate.pdf

page 1, on the bottom

that

e^{\phi^* a } f(a^{\dagger} , a ) = f(a^{\dagger} + \phi^*, a) e^{\phi^* a }

I have tried to prove this, writing both as taylor series, but the problem is to understand the "hint" :(

For the benefit of other readers, this pdf performs a quick derivation of the
coherent state path integral (in which a coherent state resolution of unity is used
between time slices rather than the usual resolutions using momentum and position
eigenstates).

The "hint" is

Use the fact that a acts like \partial/\partial a^\dagger, (...),

which refers to this trick:

<br /> [a, g(a^\dagger)] ~=~ \frac{\partial g(a^\dagger)}{\partial a^\dagger}<br />

as may be shown by induction (perhaps modulo a sign and/or some
factors of i and \hbar, depending on one's conventions).

Start with g(a^\dagger) = a^\dagger, then progress to
g(a^\dagger) = (a^\dagger)^2, to see the pattern,
then prove it for g(a^\dagger) = (a^\dagger)^n by induction.
Then you can extend the result to any well-behaved analytic function.)

HTH.
 
ah yes now its clear! Thank you


strangerep said:
For the benefit of other readers, this pdf performs a quick derivation of the
coherent state path integral (in which a coherent state resolution of unity is used
between time slices rather than the usual resolutions using momentum and position
eigenstates).

The "hint" is



which refers to this trick:

<br /> [a, g(a^\dagger)] ~=~ \frac{\partial g(a^\dagger)}{\partial a^\dagger}<br />

as may be shown by induction (perhaps modulo a sign and/or some
factors of i and \hbar, depending on one's conventions).

Start with g(a^\dagger) = a^\dagger, then progress to
g(a^\dagger) = (a^\dagger)^2, to see the pattern,
then prove it for g(a^\dagger) = (a^\dagger)^n by induction.
Then you can extend the result to any well-behaved analytic function.)

HTH.
 

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