# Is there a simple way of finding the eigenstates of the creation and annihilation operator in QM?

How can I find the eigenstates of creation and annihilation operator in QM?

My attempt:

Such eigenstate will obey: $$a^{\dagger} |\psi \rangle = \alpha |\psi \rangle.$$

We can expand $|\psi \rangle$ in terms of the quantum SHM eigenstates: $|\psi \rangle = \sum_{n=0}^{\infty} c_n |n\rangle$.

Knowing the action of the creation operation of quantum SHM eigenmodes ($a^{\dagger}|n\rangle = \sqrt{n+1}|n+1\rangle)$:

$$a^{\dagger} |\psi \rangle = a^{\dagger} \sum_{n=0}^{\infty} c_n |n\rangle = \sum_{n=0}^{\infty} c_n \sqrt{n+1}|n+1\rangle$$

from which the state $|0\rangle$ is now missing, so it will never be equal to the RHS of the first expression, $\alpha |\psi\rangle = \sum_{n=0}^{\infty} \alpha c_n |n\rangle$.

• The creation operator cannot possibly have eigenstates. The eigenstates of the annihilation operator are called "coherent states". Google it :) Commented Dec 30, 2014 at 23:52
• This is no surprise, as $a$ and $a^\dagger$ are not self-adjoint Commented Dec 30, 2014 at 23:57
• …but see this Commented Sep 1, 2021 at 17:40

Write an arbitrary state as

$$|\Psi\rangle = \sum_{n=0}^{\infty} c_n |n\rangle \,.$$

Now apply the raising operator

\begin{align} a^\dagger |\Psi\rangle &= a^\dagger \sum_{n=0}^{\infty} c_n |n\rangle \\ &= \sum_{n=0}^{\infty} c_n \sqrt{n+1} |n+1\rangle \\ &= \sum_{n=1}^{\infty} c_{n-1} \sqrt{n} |n\rangle \end{align}

If $$|\Psi\rangle$$ is an eigenstate of $$a^\dagger$$ with eigenvalue $$\alpha$$ then we have

$$\sum_{n=0}^{\infty} \alpha c_n|n\rangle = \sum_{n=1}^\infty c_{n-1} \sqrt{n}|n \rangle \, .$$

You already got this far. Indeed, the only solution to this equation is $$c_n=0$$ for all $$n$$. Therefore, there is no eigenstate of $$a^\dagger$$.

The eigenstates of $$a$$, which are called "coherent states" are given by

$$|\alpha \rangle = e^{-|\alpha|^2/2}\sum_{n=0}^\infty \frac{\alpha^n}{\sqrt{n!}}|n\rangle \, .$$ You can check easily by applying $$a$$ to $$|\alpha \rangle$$ that $$|\alpha \rangle$$ is an eigenstate of $$a$$.

• Can you please explain why $c_{n}$ =0 for all n, is the only solution for creation operator case Commented Jan 23, 2018 at 18:25
• @SSP_user5275 The right hand side of the equation has no $|0\rangle$ term, so the left hand side must also have no $|0\rangle$ term, and so $c_0=0$. Now consider the $|1\rangle$ term and we get $c_1 = c_0 \sqrt{1} = 0$. Repeat this argument for all terms. Commented Jan 23, 2018 at 21:39
• Did you miss a factor of $\alpha$ on the LHS below "If |Ψ⟩ is an eigenstate of 𝑎† with eigenvalue 𝛼 then we have"? It doesn't change the conclusion I think, it's just that one must treat $\alpha \neq 0$ and $\alpha = 0$.
– EE18
Commented Apr 7, 2023 at 18:51
• Notice that the starting index of the sum is 1 not 0. Commented Apr 8, 2023 at 1:08
• @EE18 yes, fixed now. Commented Apr 11 at 14:27