Throughout the 1920s scientists searched for the neutron but without
success.
One of the troubles was that the particle was electrically neutral.
Subatomic particles could be detected in a variety of ways, but every
single way (right down to the present time) makes use of their electric
charge. The electric charge of a speeding subatomic particle either
repels electrons or attracts them. In either case, electrons are knocked
off atoms that are encountered by the speeding subatomic particle.
The atoms with electrons knocked off are now positively charged ions.
Droplets of water vapor can form about these ions, or a bubble of gas
can form, or a spark of light can be seen. The droplets, the bubbles,
and the light can all be detected one way or another and the path of the
subatomic particle could be followed by the trail of ions it left
behind. Gamma rays, though they carry no charge, are a wave form capable
of ionizing atoms.
All the particles and rays that can leave a detectable track of ions
behind are called “ionizing radiation” and these are easy to detect.
The hypothetical proton-electron combination, however, which was neither
a wave form nor a charged particle was not expected to be able to ionize
atoms. It would wander among the atoms without either attracting or
repelling electrons and would therefore leave the atomic structure
intact. Its pathway could not be followed. In short, then, the neutron
was, so to speak, invisible, and the search for it seemed a lost cause.
And until it was found, the proton-electron theory of nuclear structure,
whatever its obvious deficiencies with respect to nuclear spin, remained
the only one to work with.
Then came 1930. The German physicist Walther Wilhelm Georg Bothe
(1891-1957) and a co-worker, H. Becker, were bombarding the light metal,
beryllium, with alpha particles. Ordinarily, they might expect protons
to be knocked out of it, but in this case no protons appeared. They
detected some sort of radiation because something was creating certain
effects while the alpha particles were bombarding the beryllium but not
after the bombardment ceased.
[Illustration: _Walther W. G. Bothe_]
To try to determine something about the properties of this radiation,
Bothe and Becker tried putting objects in the way of the radiation. They
found the radiation to be remarkably penetrating. It even passed through
several centimeters of lead. The only form of radiation that was known
at that time to come out of bombarded matter with the capacity of
penetrating a thick layer of lead was gamma rays. Bothe and Becker,
therefore, decided they had produced gamma rays and reported this.
In 1932 the Joliot-Curies repeated the Bothe-Becker work and got the
same results. However, among the objects they placed in the path of the
new radiation, they included paraffin, which is made up of the light
atoms of carbon and hydrogen. To their surprise, protons were knocked
out of the paraffin.
Gamma rays had never been observed to do this, but the Joliot-Curies
could not think what else the radiation might be. They simply reported
that they had discovered gamma rays to be capable of a new kind of
action.
[Illustration: _James Chadwick_]
Not so the English physicist James Chadwick (1891- ). In that same
year he maintained that a gamma ray, which possessed no mass, simply
lacked the momentum to hurl a proton out of its place in the atom. Even
an electron was too light to do so. (It would be like trying to knock a
baseball off the ground and into the air by hitting it with a ping-pong
ball.)
Any radiation capable of knocking a proton out of an atom had to consist
of particles that were themselves pretty massive. And if one argued like
that, then it seemed that the radiation first observed by Bothe and
Becker had to be the long-sought-for proton-electron combination.
Chadwick used Harkins’ term, neutron, for it and made it official. He
gets the credit for the discovery of the neutron.
Chadwick managed to work out the mass of the neutron from his
experiments and by 1934 it was quite clear that the neutron was more
massive than the proton. The best modern data have the mass of the
proton set at 1.007825, and that of the neutron just a trifle greater at
1.008665.
The fact that the neutron was just about as massive as the proton was to
be expected if the neutron were a proton-electron combination. It was
also not surprising that the isolated neutron eventually breaks up,
giving up an electron and becoming a proton. Out of any large number of
neutrons, half have turned into protons in about 12 minutes.
Nevertheless, although in some ways we can explain the neutron by
speaking of it as though it were a proton-electron combination, it
really is not. A neutron has a spin of ½ while a proton-electron
combination would have a spin of either 0 or 1. The neutron, therefore,
must be treated as a single uncharged particle.