Solve Hamiltonian for 1-Electron Atom: Find Energy & Normalization Constant

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SUMMARY

The discussion focuses on solving the Hamiltonian for a one-electron atom with nuclear charge Z, specifically using the wavefunction Ψ1s = Ne-Zr. Participants confirm that this wavefunction is an eigenfunction of the Hamiltonian H = -∇²/2 - Z/r. The energy corresponding to this eigenfunction is derived from the Hamiltonian, and the normalization constant N is calculated through the integral N² ∫ Ψ* Ψ dx = 1. Participants clarify that the term -Z/r must be included in the Hamiltonian application to accurately find the energy.

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For an atom with one electron and nuclear charge of Z, the Hamiltonian is:

H=-~\frac{\nabla^{2}}{2}~- ~\frac{Z}{r}~

1) show that the wavefunction:

\Psi_{1s}=Ne^{-Zr}

is an eigenfunction of the Hamiltonian

2) find the corresponding energy

3) find N, the normalisation constant

In spherical polar coordinates:

\nabla^{2}\Psi_{1s}=~\frac{1}{r^{2}}~(~\frac{d}{dr}~[r^{2}~\frac{d\Psi_{1s}}{dr}])by applying H to the wavefunction, i think I've shown that it's an eigenfunction:

1)

H\Psi_{1s}=~\frac{-Z^{2}r^{2}}{2}~Ne^{-zr} - ~\frac{Z}{r}~

H\Psi=n\Psi

where n is the eigenvalue, and the bit on the end:

- ~\frac{Z}{r}~

doesn't matter right, I've still shown it's an eigenvalue?

2)

to find the corresponding energy, don't I need to know N first?

3)

to find N, am I right in thinking:

N^{2} \int \Psi* \Psi dx = 1

N^{2} \int e^{-2zr} dx = 1

~\frac{-N^{2}}{2z}~e^{-2zr}=1

N=\sqrt{~\frac{-2}{e^{-2zr}}~}

but i think i must have gone wrong somewhere, i mean that doesn't look right. Once I've found N, how do i find the corresponding energy do i just plug N into:H\Psi_{1s}=~\frac{-Z^{2}r^{2}}{2}~Ne^{-zr} - ~\frac{Z}{r}~

ie, H\Psi_{1s} = the corresponding energy?

i'd appreciate any help, thanks
 
Physics news on Phys.org
You haven't multiplied

\frac{Z}{r}

right, it should be

\frac{Z}{r}~Ne^{-Zr}
 

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