What is the Effect of the Number Operator on a Given Wavefunction?

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SUMMARY

The discussion focuses on the effect of the number operator, denoted as ##\hat N = \hat a^\dagger \hat a##, on the wavefunction ##\psi_\alpha = Ne^{\alpha \hat a^\dagger}\phi_0##, where ##N = e^{-\frac{1}{2}|\alpha|^2}## is the normalization factor. The solution involves applying the number operator to the wavefunction, resulting in the expression ##\hat N \psi_\alpha = N \sum_{n=0}^\infty \frac{\alpha^{n}}{n!}n(\hat a^\dagger)^{n}\phi_0##. The discussion highlights the need to simplify the summation and suggests that understanding the commutation relations between ##\hat{a}## and ##\hat{a}^\dagger## is crucial for further progress.

PREREQUISITES
  • Understanding of quantum mechanics, specifically wavefunctions and operators.
  • Familiarity with creation and annihilation operators, ##\hat a## and ##\hat a^\dagger##.
  • Knowledge of normalization techniques in quantum states.
  • Basic grasp of series expansions and summation techniques.
NEXT STEPS
  • Study the commutation relations between creation and annihilation operators.
  • Learn about the properties of exponential operators in quantum mechanics.
  • Explore the concept of coherent states and their relation to the wavefunction ##\psi_\alpha##.
  • Investigate techniques for simplifying infinite series in quantum mechanics.
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Students and researchers in quantum mechanics, particularly those studying quantum harmonic oscillators and the application of number operators in wavefunction analysis.

doggydan42
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Homework Statement


Consider the state
$$\psi_\alpha = Ne^{\alpha \hat a^\dagger}\phi_0, $$
where ##\alpha## can be complex, and ##N = e^{-\frac{1}{2}|\alpha|^2}## normalizes ##\psi_\alpha##.

Find ##\hat N \psi_\alpha##.

Homework Equations


$$\hat N = \hat a^\dagger \hat a$$
$$\hat a\phi_n = \sqrt{n}\phi_{n-1}$$
$$\hat a^\dagger = \sqrt{n+1}\phi_{n+1}$$
$$\hat a \psi_\alpha = \alpha \psi_\alpha$$
$$\phi_n = \frac{1}{\sqrt{n!}}(\hat a^\dagger)^n \phi_0$$

The Attempt at a Solution


First applying ##\hat a## gives
$$\hat N \psi_\alpha = \hat a ^\dagger \alpha \psi_\alpha$$
Expanding the exponential gives
$$\alpha N \sum_{n=0}^\infty \frac{\alpha^n}{n!}(\hat a ^\dagger)^{n+1}\phi_0 = N \sum_{n=0}^\infty \frac{\alpha^{n+1}}{n!}(\hat a ^\dagger)^{n+1}\phi_0 = N \sum_{n=1}^\infty \frac{\alpha^{n}}{(n-1)!}(\hat a ^\dagger)^{n}\phi_0 = N \sum_{n=1}^\infty \frac{\alpha^{n}}{n!}n(\hat a ^\dagger)^{n}\phi_0$$

Because at n = 0 the sum becomes 0,
$$\hat N \psi_\alpha = N \sum_{n=0}^\infty \frac{\alpha^{n}}{n!}n(\hat a ^\dagger)^{n}\phi_0$$

From here, I am unsure of how to simplify the summation.
 
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There's several typos or errors in the Relevant equations part... I also think that the commutator of ##\hat{a}## and ##\hat{a}^\dagger## may be needed in this problem.

Also, note that ##\frac{1}{n!} = \frac{1}{\sqrt{n!}\sqrt{n!}}##, which allows you to convert the ##\phi_0## in the last equation to ##\phi_n##.
 
Last edited:

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