# Delta Function Bound State

• AlexChandler
So, in other words, the coefficients c1 and c2 are telling us that there is a probability of finding the energy of the bound state, but there is more to the equation than that.f

## Homework Statement

A particle moves in one dimension in the delta function potential V= αδ(x). (where that is an 'alpha' ... not 'a')
An initial wave function is given
$$\Psi = A(a^2-x^2)$$ for x between -a and a and Psi=0 anywhere else
What is the probability that an energy measurement will yield something other than:
$$E=\frac{-m\alpha^2}{2\hbar^2}$$

note: when we solve the delta function potential problem, we find (for E<0) that there is only one bound state, and only one allowed energy: and that is exactly the one shown above.

## Homework Equations

$$c_n = \int \Psi_n^* \Psi(x,0) dx$$

$$P(E_n) = abs(c_n)^2$$

## The Attempt at a Solution

At first I was sure that since there is only one bound state in the delta function potential problem, and only one allowed energy, that the probability of measuring another energy should be zero. But when I calculate the coefficient c1, I do not get 1, i get something like .913 and then c1 squared is about .83 which would then be the probability of measuring the bound state energy.
This is what is confusing me. If c1 is not equal to 1, then there must be some other c's with other eigenfunctions that must be combined linearly to produce the given initial wave function. But there is only one energy eigenfunction, so what are these other functions??
And if there is only one energy eigenstate, is it possible to measure an energy other than the energy of the eigenstate?
Thank you

there is only one bound state

Yes.
and only one allowed energy

Are you sure?

We solved the schrodinger equation and found only one bound state with a corresponding energy. What we have done before is to expand a given state in terms of energy eigenstates, and the the constants in the summation give a probability density for the energy. But if we do such an expansion, since there is only one eigenstate, wouldn't its c value have to be 1? If not, then what other functions are we including in the linear combination?

Is the bound state the only energy eigenstate?

i don't know of any others..

The key word is bound.

If anybody has an explanation I would be happy to hear it. I have turned in the homework assignment already and decided it makes most sense to just calculate the c value for the bound state, and say

$$P(E \neq E_1 ) = 1 - |c_1|^2 = .17$$

What I am wondering about is how to express the state as a combination of eigenstates. Is it c1 times the bound state, and then plus some integral over scattering states?

What I am wondering about is how to express the state as a combination of eigenstates. Is it c1 times the bound state, and then plus some integral over scattering states?

Yes. From Quantum Mechanics by Robinettt
There is a discrete bound spectrum for E<0 (actually only one state), but there is a continuum of unbound states with E>0 ... The discrete and continuous states, taken together, form a complete set from which any admissible wavefunction can be constructed; the bound state solutions, by themselves, are not sufficient.

Aha! Thank you