230 ERWIN SCHRÖDINGER
only certain distances, and certain
energy levels, would be stable.
However, de Broglie’s solution relied
on treating the matter wave as a
one-dimensional wave trapped in
orbit around the nucleus—a full
description would need to describe
the wave in three dimensions.
The wave equation
In 1925, three German physicists,
Werner Heisenberg, Max Born, and
Pascual Jordan, tried to explain the
quantum jumps that occurred in
Bohr’s model of the atom with a
method called matrix mechanics,
in which the properties of an atom
were treated as a mathematical
system that could change over
time. However, the method could
not explain what was actually
happening inside the atom, and
its obscure mathematical language
did not make it very popular.
A year later, an Austrian
physicist working in Zurich, Erwin
Schrödinger, hit upon a better
approach. He took de Broglie’s
wave-particle duality a step further
and began to consider whether
there was a mathematical equation
of wave motion that would describe
how a subatomic particle might
move. To formulate his wave
equation, he began with the laws
governing energy and momentum
in ordinary mechanics, then
amended them to include the
Planck constant and de Broglie’s
law connecting the momentum of
a particle to its wavelength.
When he applied the resulting
equation to the hydrogen atom,
it predicted exactly the specific
energy levels for the atom that had
been observed in experiments. The
equation was a success. But one
awkward issue remained, because
no one, not even Schrödinger, knew
exactly what the wave equation
really described. Schrödinger tried
to interpret it as the density of
electric charge, but this was not
entirely successful. It was Max
Born who eventually suggested
what it really was—it was a
probability amplitude. In other
words, it expressed the likelihood
of a measurement finding the
electron in that particular place.
Unlike matrix mechanics, the
Schrödinger wave equation or
“wave function” was embraced by
physicists, although it threw open
a whole range of wider questions
about its proper interpretation.
Pauli’s exclusion principle
Another important piece of the
puzzle fell into place in 1925
courtesy of another Austrian,
Wolfgang Pauli. In order to describe
why the electrons within an atom
did not all automatically fall directly
into the lowest possible energy
state, Pauli developed the
exclusion principle. Reasoning
that a particle’s overall quantum
state could be defined by a certain
number of properties, each with a
fixed number of possible discrete
values, his principle stated
that it was impossible for two
particles within the same system
to have the same quantum
state simultaneously.
In order to explain the pattern
of electron shells that was apparent
from the periodic table, Pauli
calculated that electrons must be
described by four distinct quantum
numbers. Three of these—the
principal, azimuthal, and magnetic
quantum numbers—define the
electron’s precise place within
the available orbital shells and
subshells, with the values of the
A classic illustration of wave-particle
duality involves firing electrons from a
“gun” through a barrier with two slits in
it. If electrons are allowed to build up over
time, an interference pattern forms, just
as it would for light waves.
Interference
pattern
Narrow slits
Electrons
Gun