Inferring the Principal Quantum Number from a Given Wave Function

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SUMMARY

This discussion focuses on inferring the principal quantum number from a given wave function of the hydrogen atom, specifically using the wave function \(\psi_{nlm} = \frac{1}{{\sqrt{4\pi}}}\left(\frac{1}{{2a}}\right)^{3/2}\left(2 - \frac{r}{a}\right)e^{-r/2a}\). The principal quantum number for this wave function is determined to be 2, based on the zero-crossing method, where the number of zeroes corresponds to the quantum number. The energy eigenvalue is calculated using the Hamiltonian \(H = -\frac{{\hbar^2}}{{2m}}\nabla^2 - \frac{{e^2}}{r}\), leading to the conclusion that the integration method is time-consuming and may not be practical for exam conditions.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave functions.
  • Familiarity with the hydrogen atom's Hamiltonian and energy eigenvalues.
  • Knowledge of zero-crossing rules in wave functions.
  • Ability to perform triple integrals in quantum mechanics.
NEXT STEPS
  • Study the radial wave equation and its implications for quantum numbers.
  • Learn about the Rodrigues formula for generating orthogonal polynomials in quantum mechanics.
  • Explore alternative methods for determining quantum numbers from wave functions.
  • Review the properties of wave functions in quantum mechanics, focusing on zero-crossings and their significance.
USEFUL FOR

Graduate physics students, quantum mechanics enthusiasts, and anyone preparing for exams in quantum theory will benefit from this discussion.

Useong
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Hi, I am new here. I am a graduate student of department of physics at some university in Korea. If there is any wrong in my english, I will apologize in advance. I am preparing for my qualifying exam that is going to be held on next month.

Homework Statement


The question is very simple as I stated in the title. "Can you infer the principal quantum number from a given wave function of the hydrogen atom?" Not by memorizing but by logical deduction. I think no one can memorize all of the wave functions of the hydrogen atom.

Homework Equations


For example, you are given this wave function [tex]\psi _{nlm} = \frac{1}{{\sqrt {4\pi } }}\left( {\frac{1}{{2a}}} \right)^{3/2} \left( {2 - \frac{r}{a}} \right)e^{ - r/2a}[/tex]
where[tex]a = \frac{\hbar }{{me^2 }}[/tex]. Of cource, you may know the Hamiltonian that is composed of the kinetic term and the Coulomb potential.
[tex]H = - \frac{{\hbar ^2 }}{{2m}}\nabla ^2 - \frac{{e^2 }}{r}[/tex]
The principal quantum number of above wave equation is 2. But how would you infer it?


The Attempt at a Solution


I tried this method. I know the energy eigenvalue is given by
[tex]E_n = - \frac{{e^2 }}{{2a}}\frac{1}{{n^2 }}[/tex]

So, when I carried out the integration to find the energy eigenvalue, I could obtain

[tex]E_n = \iiint {d^3 r\psi _{nlm}^ * \hat H\psi _{nlm} } = - \frac{{e^2 }}{{2a}}\frac{1}{{\left( 2 \right)^2 }}[/tex]
and therefore I could conclude n=2. But the method took me so long time that it may fail me if I meet this problem in exam time. So if you know any better methods to solve this problem, please let me know. Please enlighten me. Thanks a lot.
 
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The is one zero-crossing for the given function, at r=2a. So the principle quantum number is 2.

For n=1, there are no zeroes.
For n=2, there is 1 zero.
For n=3, there are 2 zeroes.
etc. etc

(At least, that's the case when L=M=0. It has been awhile since I had this, so nonzero L and M might or might not change the zero-crossing rule.)
 

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