Chadwick, James. "Possible Existence of a Neutron", in Nature, 27 February 1932. volume 129. This revolutionary contribution appears as a Letter to the Editor, in 1.25 columns, on page 312 of this issue of the journal. And in the "tradition" of the Alpher-Bethe-Gamow paper (the great paper on the Big Bang, appearing on April 1st 1948 in the Physical Review), it is another instance of a major announcement being made as a "simple" letter to the editor. (Well, in the case of scientific letters, this is really just a shorter, quicker-to-publication avenue to publication, and not much at all like a letter-to-the-editor of the NYT. Still, the description has a nice ring to it.) This was the description of the neutron made after only about two weeks of experimentation.
We offer a fine copy of the full half-year of this journal, bound in cloth, with the Chadwick appearing on page 312. $800
"In 1932, Chadwick made a fundamental discovery in the domain of
nuclear science: he proved the existence of neutrons -
elementary particles devoid of any electrical charge. In contrast
with the helium nuclei (alpha rays) which are charged, and
therefore repelled by the considerable electrical forces present
in the nuclei of heavy atoms, this new tool in atomic
disintegration need not overcome any electric barrier and is
capable of penetrating and splitting the nuclei of even the
heaviest elements. Chadwick in this way prepared the way towards
the fission of uranium 235 and towards the creation of the atomic
bomb."--NobelPrize.org
His next paper1--and perhaps the more famous of the two--appeared a few months later in May and contained the proof of the existence of the neutron, and was an epochal achievement int he understanding of the nucleus.
For this epoch-making discovery he was awarded the Hughes
Medal of the Royal Society in 1932, and then the Nobel
Prize for Physics in 1935. I think he may be the only recipient of the award who was also at one time a POW. (1914-1918 in Chadwick's case, going from there to a PhD at Cambridge in 1921 and then to Rutherford's assistant shortly thereafter.)
Notes:
- Chadwick, J. (1932). "The Existence of a Neutron". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences136 (830): 692. doi:10.1098/rspa.1932.0112. Another paper appeared int he next year, (1933). "Bakerian Lecture. The Neutron". Proceedings of the Royal Society A: Mathematical, Physical and Engineering
The full text of the paper, below:
James Chadwick
Nature, p. 312 (Feb. 27, 1932)
It has been shown by Bothe and others that beryllium when bombarded
by a-particles of polonium emits a radiation
of great penetrating power, which has been an absorption coefficient in
lead of about 0.3 (cm)¯1. Recently Mme. Curie-Joliot and
M. Joliot found, when measuring the ionisation produced by this beryllium
radiation in a vessel with a thin window, that the ionisation increased
when matter containing hydrogen was placed in front of the window. The
effect appeared to be due to the ejection of protons with velocities up
to a maximum of nearly 3 x 109 cm. per sec. They suggested that
the transference of energy to the proton was by a process similar to the
Compton effect, and estimated that the beryllium radiation had a quantum
energy of 50 x 106 electron volts.
I have made some experiments using the valve counter to examine the
properties of this radiation excited in beryllium. The valve counter consists
of a small ionisation chamber connected to an amplifier, and the sudden
production of ions by the entry of a particle, such as a proton or a-particle,
is recorded by the deflexion of an oscillograph. These experiments have
shown that the radiation ejects particles from hydrogen, helium, lithium,
beryllium, carbon, air, and argon. The particles ejected from hydrogen
behave, as regards range and ionising power, like protons with speeds up
to about 3.2 x 109 cm. per sec. The particles from the other
elements have a large ionising power, and appear to be in each case recoil
atoms of the elements.
If we ascribe the ejection of the proton to a Compton recoil from a
quantum of 52 x 106 electron volts, then the nitrogen recoil
atom arising by a similar process should have an energy not greater than
about 400,000 volts, should produce not more than about 10,000 ions, and
have a range in air at N.T.P. of about 1.3 mm. Actually, some of the recoil
atoms in nitrogen produce at least 30,000 ions. In collaboration with Dr.
Feather, I have observed the recoil atoms in an expansion chamber, and
their range, estimated visually, was sometimes as much as 3 mm at N.T.P.
These results, and others I have obtained in the course of the work,
are very difficult to explain on the assumption that the radiation from
beryllium is a quantum radiation, if energy and momentum are to be conserved
in the collisions. The difficulties disappear, however, if it be assumed
that the radiation consists of particles of mass 1 and charge 0, or neutrons.
The capture of the a-particle by the Be9
nucleus may be supposed to result in the formation of a C12
nucleus and the emission of the neutron. From the energy relations of this
process the velocity of the neutron emitted in the forward direction may
well be about 3 x 109 cm. per sec. The collisions of the neutron
with the atoms through which it passes give rise to the recoil atoms, and
the observed energies of the recoil atoms are in fair agreement with this
view. Moreover, I have observed that the protons ejected from hydrogen
by the radiation emitted in the opposite direction to that of the exciting
a-particle appear to have a much smaller range
than those ejected by the forward radiation. This again receives a simple
explanation of the neutron hypothesis.
If it be supposed that the radiation consists of quanta, then the capture
of the a-particle by the Be9 nucleus
will form a C13 nucleus. The mass defect of C13 is
known with sufficient accuracy to show that the energy of the quantum emitted
in this process cannot be greater than about 14 x 106 volts.
It is difficult to make such a quantum responsible for the effects observed.
It is to be expected that many of the effects of a neutron in passing
through matter should resemble those of a quantum of high energy, and it
is not easy to reach the final decision between the two hypotheses. Up
to the present, all the evidence is in favour of the neutron, while the
quantum hypothesis can only be upheld if the conservation of energy and
momentum be relinquished at some point.
J. Chadwick.
Cavendish Laboratory,
Cambridge, Feb. 17.