Displacement Operator definition

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The discussion centers on the equivalence of two definitions of the displacement operator in quantum mechanics. The first definition is the standard form, while the second arises from the Fock state decomposition of a coherent state. It is clarified that the two definitions are not equal as operators, but they yield the same result when acting on the vacuum state due to the Baker-Campbell-Hausdorff theorem. The first definition is preferred for its unitary properties, while both forms have their applications. The conversation concludes with an acknowledgment of the importance of the identity term in the Taylor expansion of the exponential function.
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
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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