The hydrogen atom has special significance in quantum mechanics as a simple physical system for which an exact solution to the Schrödinger equation exists, from which the experimentally observed frequencies and intensities of the hydrogen spectral lines can calculated.
In 1913, Niels Bohr had deduced the spectral frequencies of the hydrogen atom making several assumptions (see The Bohr Model). The results of Bohr for the frequencies and underlying energy values are confirmed by the full quantummechanical analysis which uses the Schrödinger equation, as was shown in 1925/26. The full analysis goes further, because it also yields the shape of the electron's wave function ("orbital") for the different possible quantummechanical states. This allows to determine the intensity of spectral lines (which correspond to transitions between these states), among other things. In addition, the full analysis is applicable also to more complicated atoms with more than one electron, as well as molecules etc. However, in all of these cases approximations have to be made and computer calculations are usually necessary.
The solution of the Schrödinger equation for the hydrogen atom uses the fact that the Coulomb potential[?] produced by the nucleus is isotropic (it only depends on the distance to the nucleus). Although the resulting energy eigenfunctions[?] (the "orbitals") are not necessarily isotropic themselves, their dependence on the angular coordinates[?] follows completely generally from this isotropy of the underlying potential: The states are not only eigenstates[?] of the Hamiltonian, but also eigenstates of the angular momentum operator[?]. This corresponds to the fact that angular momentum is conserved[?] in the motion of the electron around the nucleus. Therefore, the energy eigenstates may be classified by two angular momentum quantum numbers[?], l and m (integer numbers). The "angular momentum" quantum number l=0,1,2,... determines the magnitude of the angular momentum. The "magnetic" quantum number m=l,..,+l determines the projection of the angular momentum on the (arbitrarily chosen) zaxis.
In addition, the radial dependence of the wave functions has to be found. It is only here that the details of the 1/r Coulomb potential enter (leading to Laguerre polynomials[?] in r). This leads to a third quantum number, the "main" quantum number n=1,2,3,... Note that the angular momentum quantum number can run only up to n1, i.e. l=0,1,...,n1.
Due to angular momentum conservation, states of the same l but different m have the same energy (this holds for all problems with rotational symmetry[?]). In addition, for the hydrogen atom, the states of the same n are also degenerate (i.e. they have the same energy); but this is a specialty and it is no longer true for more complicated atoms which have an (effective) potential differing from the form 1/r (due to the presence of the inner electrons shielding the nucleus potential).
Taking into account the spin of the electron adds a last quantum number, the projection of the electrons spin along the z axis, which can take on two values. Therefore, any eigenstate of the electron in the hydrogen atom is described fully by four quantum numbers. According to the usual rules of quantum mechanics, the actual state of the electron may be any superposition of these states. This explains also why the choice of zaxis for the quantization of angular momentum is immaterial: An orbital of given l and m' obtained for another preferred axis z' can always be represented as a suitable superposition of the various states of different m (but same l) that have been obtained for z.
The picture below shows the first few hydrogen atom orbitals (energy eigenfunctions). These are crosssections of the probability density[?] that are colorcoded (black=zero density, white=highest density). The angular momentum quantum number l is denoted in each column, using the usual spectroscopic letter code ("s" means l=0; "p": l=1; "d": l=2). The main quantum number n (=1,2,3,...) is marked to the right of each row. For all pictures the magnetic quantum number m has been set to 0, and the crosssectional plane is the xz plane (z is the vertical axis). The probability density in threedimensional space is obtained by rotating the one shown here around the zaxis.
The "ground state", i.e. the state of lowest energy, in which the electron is usually found, is the first one, the "1s" state (n=1,l=0).
Click here to view an image with more orbitals (up to higher numbers n and l).
Note the number of black lines that occur in each but the first orbital. These are "nodal lines[?]" (which are actually nodal surfaces[?] in three dimensions). Their total number is always equal to n1.
There are several important effects that are neglected by the Schrödinger equation and which are responsible for certain small but measurable deviations of the real spectral lines from the predicted ones:
Both of these features (and more) are incorporated in the relativistic Dirac equation, whose predictions come still closer to experiment. It can still be solved exactly for the hydrogen atom. The resulting states now must be classified by the total angular momentum number j (arising through the coupling between electron spin and orbital angular momentum). States of the same j and the same n are still degenerate.
For these developments, it was essential that the solution of the Dirac equation for the hydrogen atom could be worked out exactly, such that any experimentally observed deviation had to be taken serious as a signal of failure of the theory.
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