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

In summary, the Hamiltonian for an atom with one electron and nuclear charge of Z is given by H=-~\frac{\nabla^{2}}{2}~- ~\frac{Z}{r}~. By applying H to the wavefunction \Psi_{1s}=Ne^{-Zr}, it is shown to be an eigenfunction with an eigenvalue of n. The corresponding energy can be found by plugging in the value of N into the equation for H\Psi_{1s} and solving for the energy. The normalization constant N can be found by using the equation N=\sqrt{~\frac{-2}{e^{-2zr}}~} and multiplying the expression \frac{Z}{r
  • #1
UbikPkd
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For an atom with one electron and nuclear charge of Z, the Hamiltonian is:

[tex] H=-~\frac{\nabla^{2}}{2}~- ~\frac{Z}{r}~ [/tex]

1) show that the wavefunction:

[tex]\Psi_{1s}=Ne^{-Zr}[/tex]

is an eigenfunction of the Hamiltonian

2) find the corresponding energy

3) find N, the normalisation constant

In spherical polar coordinates:

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

1)

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

[tex]H\Psi=n\Psi [/tex]

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

[tex]- ~\frac{Z}{r}~[/tex]

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:

[tex] N^{2} \int \Psi* \Psi dx = 1[/tex]

[tex]N^{2} \int e^{-2zr} dx = 1[/tex]

[tex]~\frac{-N^{2}}{2z}~e^{-2zr}=1[/tex]

[tex]N=\sqrt{~\frac{-2}{e^{-2zr}}~}[/tex]

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:[tex]H\Psi_{1s}=~\frac{-Z^{2}r^{2}}{2}~Ne^{-zr} - ~\frac{Z}{r}~[/tex]

ie, [tex]H\Psi_{1s}[/tex] = the corresponding energy?

i'd appreciate any help, thanks
 
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  • #2
You haven't multiplied

[tex]\frac{Z}{r}[/tex]

right, it should be

[tex]\frac{Z}{r}~Ne^{-Zr}[/tex]
 

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

What is a Hamiltonian in quantum mechanics?

The Hamiltonian is an operator in quantum mechanics that represents the total energy of a system. It includes both the kinetic and potential energy of the particles in the system.

Why is it important to solve the Hamiltonian for a 1-electron atom?

Solving the Hamiltonian for a 1-electron atom allows us to understand the energy levels and wavefunctions of the atom, which are crucial for understanding its behavior and properties.

How do you find the energy of a 1-electron atom?

The energy of a 1-electron atom can be found by solving the Schrödinger equation, which involves using the Hamiltonian operator to calculate the total energy of the system.

What is the normalization constant in quantum mechanics?

The normalization constant is a factor used to ensure that the wavefunction of a system is properly normalized, meaning that the probability of finding the system in any state is equal to 1.

How does solving the Hamiltonian for a 1-electron atom relate to the Bohr model?

The Bohr model of the atom was one of the first attempts to understand the energy levels of a 1-electron atom. Solving the Hamiltonian for a 1-electron atom provides a more accurate and complete understanding of these energy levels compared to the simplified Bohr model.

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