Interpreting Hydrogen Atom Wave Functions: A Question of Correctness?

AI Thread Summary
The discussion revolves around the normalization of a wave function derived from the Schrödinger equation for a hydrogen atom. The participant questions whether the constant A can be imaginary, concluding that if A is complex, it leads to a contradiction in normalization. The conversation highlights the importance of ensuring that the radial and spherical harmonic functions are correctly accounted for in the normalization process. There is also speculation about potential errors in the textbook problem, suggesting that it may contain a typo. Overall, the participants emphasize the necessity of adhering to normalization conditions for wave functions in quantum mechanics.
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Homework Statement



I solved the Schrödinger equation, obtaining a wave function in terms of Radial and the spherical harmonics as follows:

$$Ψ(r,0)= AR_{10} Y_{00} + \sqrt{\frac23} R_{21} Y_{10} + \sqrt{\frac23} R_{21} Y_{11} - \sqrt{\frac23} R_{21} Y_{1,-1}$$


Homework Equations




The Attempt at a Solution


The constant A is equal to i; is this result right or not?
 
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Please provide a problem statement.
But I doubt the constant is going to be imaginary - what is your reasoning?
 
The states is more to write but I make a print screen.

http://www.gfxroad.com/print-wf
 
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I can see why you didn;t want to write that down ;)
See the line below the equation where it says "where A is a real constant..."?
Your question:
The constant A is equal to i; is this result right or not?
... is answered.

You seem to be trying to answer part (b).
What is the condition that must be satisfied for ##\psi(\vec r,0)## to be normalized?
 
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∫ψψ*dτ=1
 
Very good ... imagine you had ##\psi = a\psi_a + b\psi_b## ... where ##\psi_a## and ##\psi_b## are already normalized. In order for ##\psi## to be normalized, ##a## and ##b## need to satisfy a condition ... what is it?
 
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a2+b2=1
 
Well done.
Technically: ##a^*a+b^*b=1## in case you have complex coefficients.

Now imagine you have:

##\qquad \psi = a\psi_a + \sqrt{\frac{2}{3}}\psi_b + \sqrt{\frac{2}{3}}\psi_c - \sqrt{\frac{2}{3}}\psi_d##

... now your problem is that to get ##|\psi|^2=1## it looks like you have ##a^2+2=1 \implies a=\sqrt{-1}##

But you are told that ##a## is real so this is a contradiction.
Anyway, if ##a=i##, then ##a^*a= (-i)i = -i^2=1## not the -1 you were looking for.

In fact, is there even a solution for ##a^*a=-1##?

Therefore - what does this tell you about your approach?
Did you properly account for the R and Y functions?
i.e. is ##\psi_{nlm}=R_{nl}Y_{lm}## normalized already?
... did you do part (a) correctly?
 
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Yes, I thought part a was done correctly like:
http://www.gfxroad.com/print2
 
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  • #10
Yeah, I'm getting the same thing ... I have a nagging feeling there's a wrinkle here I'm missing but on the face of it the textbook problem has no solution.

It may be that the text-book has a typo.
 
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  • #11
What's about e branch, is there any starting point or equation for this, because I don't know where can I starting. The other branches solved correctly.
 
  • #12
For (e) ##\text H\psi_{nlm}=E_n\psi_{nlm}##

What do you mean "correctly"? Do you have model answers?
 

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