Coherent States: Ʃ(|α|2)n = 1?

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    Coherent States
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Discussion Overview

The discussion revolves around the normalization condition of coherent states in quantum mechanics, specifically whether the sum Ʃ(|α|²)ⁿ equals 1 when summed from n=0 to infinity. The scope includes theoretical aspects of quantum states and normalization procedures.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions the truth of the statement Ʃ(|α|²)ⁿ = 1, seeking clarification on its validity.
  • Another participant explains the normalization of coherent states, noting that the norm of the coherent state involves an exponential function and that normalization can be achieved by a specific choice of the constant c.
  • A different normalization condition is presented for an alternative state |tilde{α}⟩, suggesting that under certain definitions, the sum does equal 1.
  • A later reply introduces a point of contention regarding the definition of α, indicating that it may not be the complex eigenvalue of the annihilation operator, which could affect the interpretation of the normalization condition.

Areas of Agreement / Disagreement

Participants do not reach a consensus; there are competing views regarding the normalization conditions and the definitions involved in the coherent states.

Contextual Notes

Limitations include the lack of specific references to the article mentioned, and the discussion does not resolve the implications of the different definitions of α on the normalization condition.

Hazzattack
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Hi guys,

Just a quick question, is the following statement true (it seems to be implied in the article I'm looking at);

Ʃ(|α|2)n = 1

(The sum over n=0 to infinity)

Thanks to anyone who takes a look.
 
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You don't post the reference, so I will refer to generalities. Typically the coherent state for the harmonic oscillator is written as

$$ | \alpha \rangle = c \sum_{n=0}^\infty \frac{\alpha^n}{\sqrt{n!}} | n\rangle.$$

The norm of this state is

$$\langle \alpha | \alpha \rangle = |c|^2 \sum_{n=0}^\infty \frac{|\alpha|^{2n}}{n!} = |c|^2 e^{|\alpha|^2}, $$

so we can normalize the state by choosing ##c = \exp ( - |\alpha|^2/2 )##. If we had instead written

$$ | \tilde{\alpha} \rangle = \sum_{n=0}^\infty \tilde{\alpha}^n | n\rangle,$$

then the normalization condition is indeed

$$\sum_{n=0}^\infty |\tilde{\alpha}|^{2n} =1.$$
 
Great! That's what i was hoping, but for some reason i was confusing myself. Will post the workings i was referencing later. Thanks for taking a look!
 
We have to say that in the relation of hazzattack alpha is not the complex eigenvalue of the annihilation operator..
 
Last edited:

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