Show that wave function in coordinates x,y is normalized

Crista
Messages
3
Reaction score
0

Homework Statement


A particle is described by the state of the following wave function.

wavefunction(x,y) = 30/[(a^5)(b^5)]^1/2 * x(a-x) * b(b-y)

Homework Equations


integral from 0 to i of x^n * (1-x)^m dx = (n!m!)/(n+m+1)!

The Attempt at a Solution


I know that normalizing means taking the integral from negative infinity to positive infinity of the probability density squared with respect to x, but I just don't know how to take that with respect to x and y. I tried looking at problems that involved a particle in a 2d box, but doing the math seems extremely difficult.
 
Physics news on Phys.org
I presume when you say that is the wavefunction you mean that is the wavefunction's representation in the position (X) basis.
In that case your statement equates to saying that
$$\langle x,y | \psi\rangle = \frac{30}{\sqrt{a^5+b^5}}x(a-x)b(b-y)$$
and you are asked to prove that ##\langle \psi|\psi\rangle = 1##.

What you need to do is expand ##\langle \psi|\psi \rangle= 1## in the X basis as follows:

$$\langle \psi|\psi\rangle = \int_{-\infty}^\infty \int_{-\infty}^\infty \langle \psi | x,y\rangle\langle x,y | \psi\rangle\, dy\,dx$$

Now use the fact that ##\langle u|v\rangle = \langle v|u\rangle^*## to simplify that and substitute in your function for ##\langle x,y | \psi\rangle##. You should find that the integral factorises nice and easily.

ETA: But I don't think the integrals will exist. Are you sure you wrote the function correctly? It should go to zero as ##x,y\to\pm\infty##, but what you wrote doesn't.
 
It shows now boundaries, but people have suggested that I integrate from 0->a according to x and 0->b according to y.
 
andrewkirk said:
I presume when you say that is the wavefunction you mean that is the wavefunction's representation in the position (X) basis.
In that case your statement equates to saying that
$$\langle x,y | \psi\rangle = \frac{30}{\sqrt{a^5+b^5}}x(a-x)b(b-y)$$
and you are asked to prove that ##\langle \psi|\psi\rangle = 1##.

What you need to do is expand ##\langle \psi|\psi \rangle= 1## in the X basis as follows:

$$\langle \psi|\psi\rangle = \int_{-\infty}^\infty \int_{-\infty}^\infty \langle \psi | x,y\rangle\langle x,y | \psi\rangle\, dy\,dx$$

Now use the fact that ##\langle u|v\rangle = \langle v|u\rangle^*## to simplify that and substitute in your function for ##\langle x,y | \psi\rangle##. You should find that the integral factorises nice and easily.

ETA: But I don't think the integrals will exist. Are you sure you wrote the function correctly? It should go to zero as ##x,y\to\pm\infty##, but what you wrote doesn't.
also, its (a^5)*(b^5) but the way you stated how to integrate it according to x and then y helped a lot. Not sure if the answer is correct, but I shall ask my teacher when I get it back. thank you!
 
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top