Energy Levels of Hydrogen Atom

(4.119) |

The radial eigenfunction satisfies Equation (4.118), which can be written

(4.120) |

Here, is the

which is the one-dimensional Schrödinger equation for a particle of mass moving in the

(4.122) |

The effective potential has a simple physical interpretation. The first part is the attractive Coulomb potential, and the second part corresponds to the repulsive centrifugal force.

Let

and , with

Here, it is assumed that the energy eigenvalue is negative. Equation (4.121) transforms to

Let us look for a power-law solution of the form

Substituting this solution into Equation (4.125), we obtain

(4.127) |

Equating the coefficients of gives

Now, the power-law series (4.126) must terminate at small , at some positive value of , otherwise would diverge unphysically as . This is only possible if , where the first term in the series is . There are two possibilities: or . The former predicts unphysical divergence of the wavefunction at . Thus, we conclude that , and that the first term in the series is . Note that for an state there is a finite probability of finding the electron at the nucleus, whereas for an state there is zero probability of finding the electron at the nucleus (i.e., at , except when ). Furthermore, it is only possible to obtain sensible behavior of the wavefunction as if is an integer.

For large values of , the ratio of successive terms in the series (4.126) is

(4.129) |

according to Equation (4.128). This is the same as the ratio of successive terms in the series

(4.130) |

which converges to . We conclude that as . It follows from Equation (4.124) that as . This does not correspond to physically acceptable behavior of the wavefunction, because must be finite. The only way in which we can avoid this unphysical behavior is if the series (4.126) terminates at some maximum value of . According to the recursion relation (4.128), this is only possible if

(4.131) |

where the last term in the series is . It follows from Equation (4.123) that the energy eigenvalues are quantized, and can only take the values

where

(4.133) |

is the energy of the

In summary, the properly normalized wavefunction of a hydrogen atom is written

(4.134) |

where

(4.135) |

and

(4.136) |

Here,

(4.137) |

is the

that satisfies the normalization constraint

(4.139) |

Finally, the are spherical harmonics. The restrictions on the quantum numbers are , where is a positive integer, a non-negative integer, and an integer. Incidentally, the quantum numbers , , and are conventionally referred to as the

The ground state of hydrogen corresponds to . The only permissible values of the other quantum numbers are and . Thus, the ground state is a spherically symmetric, zero angular momentum, state. The next energy level corresponds to . The other quantum numbers are allowed to take the values , or , . Thus, there are states with non-zero angular momentum. Note that the energy levels given in Equation (4.132) are independent of the quantum number , despite the fact that appears in the radial eigenfunction equation (4.138). This is a special property of a Coulomb potential.

In addition to the quantized negative energy states of the hydrogen atom, which we have just found, there is also a continuum of unbound positive energy states.