Number operator on wavefunction

In summary, we are given the state ##\psi_\alpha = Ne^{\alpha \hat a^\dagger}\phi_0## and are asked to find ##\hat N \psi_\alpha##. Using the equations ##\hat N = \hat a^\dagger \hat a## and ##\hat a \phi_n = \sqrt{n}\phi_{n-1}##, we can expand the exponential and simplify the summation to get ##\hat N \psi_\alpha = N \sum_{n=1}^\infty \frac{\alpha^{n}}{n!}n(\hat a ^\dagger)^{n}\phi_0##. However, the commutator
  • #1
doggydan42
170
18

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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  • #2
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:

What is the number operator on a wavefunction?

The number operator on a wavefunction is a mathematical operator that acts on a wavefunction to determine the number of particles present in a particular state. It is represented by the symbol "N" and is used in quantum mechanics to calculate the expected value of the number of particles in a given quantum state.

How is the number operator defined?

The number operator is defined as the product of the creation operator and the annihilation operator. In mathematical notation, it can be written as N = aa, where a is the creation operator and a is the annihilation operator. This definition allows for the calculation of the number of particles present in a state by measuring the expectation value of the number operator on the wavefunction.

What is the significance of the number operator in quantum mechanics?

The number operator is a fundamental concept in quantum mechanics as it allows for the measurement of the number of particles present in a particular state. It is also used in the study of quantum systems and their dynamics, as it is a key factor in determining the probabilities of different outcomes of measurements on the system.

How does the number operator behave under different operations?

The number operator follows specific rules when acted upon by different mathematical operations. For example, when the number operator is multiplied by a constant, the expected value of the number of particles is also multiplied by that same constant. Similarly, when the number operator is raised to a power, the expected value of the number of particles is also raised to that power.

Can the number operator have a negative value?

No, the number operator cannot have a negative value. This is because it is defined as the product of the creation and annihilation operators, and the annihilation operator always removes particles from a state, resulting in a positive value for the number of particles. In quantum mechanics, the number operator is always represented by a positive integer or zero.

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