Displacement Operator definition

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Discussion Overview

The discussion centers on the definitions of the displacement operator in quantum mechanics, specifically comparing two forms: the standard definition and one derived from the Fock state decomposition of a coherent state. Participants explore the reasoning behind the equivalence of these definitions and their implications for producing coherent states from the vacuum state.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question how the two definitions of the displacement operator, \( e^{\alpha a^{\dagger}-\alpha^* a} \) and \( e^{\frac{-|\alpha^{2}|}{2}} e^{\alpha a^{\dagger}} \), can be considered equivalent.
  • One participant suggests that while the two definitions are not equal as operators, they may yield the same result when acting on the vacuum state, referencing the Baker-Campbell-Hausdorff (BCH) theorem.
  • Another participant points out that the rightmost exponential term in the BCH expansion involves only the annihilation operator, which acts on the vacuum state to yield zero, leading to confusion about the implications.
  • A clarification is made that the exponential of zero is equal to one, which resolves the concern about obtaining zero when applying the annihilation operator to the vacuum state.

Areas of Agreement / Disagreement

Participants express differing views on the equivalence of the two definitions of the displacement operator. While some acknowledge the utility of both forms in different contexts, there is no consensus on whether one definition is preferable or more fundamental than the other.

Contextual Notes

The discussion involves assumptions related to the application of the BCH theorem and the properties of exponential operators in quantum mechanics. There are unresolved aspects regarding the specific conditions under which the equivalence holds.

Who May Find This Useful

This discussion may be useful for those studying quantum mechanics, particularly in the context of coherent states and operator algebra, as well as for individuals interested in the mathematical foundations of quantum theory.

McLaren Rulez
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Hi,

Could someone explain how the following two definitions of the displacement operator are equal? The first is the standard one

1) e^{\alpha a^{\dagger}-\alpha*a}

But what about this one? This is from a Fock state decomposition of a coherent state.

2) e^{\frac{-|\alpha^{2}|}{2}}e^{\alpha a^{\dagger}}

What is the reasoning behind not using the second equation to define the operator that acts on a vacuum state to produce a coherent state? Or if it is fine to use definition 2), then can someone help me show that the two definitions are equivalent?

Thank you
 
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McLaren Rulez said:
Could someone explain how the following two definitions of the displacement operator are equal? The first is the standard one

1) e^{\alpha a^{\dagger}-\alpha*a}

But what about this one? This is from a Fock state decomposition of a coherent state.

2) e^{\frac{-|\alpha^{2}|}{2}}e^{\alpha a^{\dagger}}

What is the reasoning behind not using the second equation to define the operator that acts on a vacuum state to produce a coherent state? Or if it is fine to use definition 2), then can someone help me show that the two definitions are equivalent?
They're not equal as operators, but if you act on the vacuum with them, e.g.,
$$e^{\alpha a^{\dagger}-\bar\alpha a} \, |0\rangle$$
you should be able to use one of the BCH theorems (Baker-Campbell-Hausdorff) -- or is it Zassenhaus? -- to convert the exponential into a product of exponentials, where the rightmost one involves only the annihilation operator, and hence leaves the vacuum unchanged.

http://en.wikipedia.org/wiki/Baker–Campbell–Hausdorff_formula

The advantage of version (1) is that its formally unitary. Both are useful in different circumstances. Try Mandel & Wolf for lots more on this.
 
Using the BCH equations, the article arrived at e^{\frac{|\alpha^{2}|}{2}}e^{\alpha a^{\dagger}}e^{\alpha^{*} a} for the displacement operator. Now, I expand the last exponential term in powers of a.

But if the rightmost one only involves the annihilation operator, then we get zero. Isn't it true that a\left|0\right\rangle = 0, not \left|0\right\rangle?
 
But if the rightmost one only involves the annihilation operator, then we get zero
It's an exponential whose exponent involves only a. And e0 = 1.
 
Oh of course! I forgot the identity term in the Taylor expansion. Thank you very much Bill_K and strangerep
 

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