 |
 |
 |
 |
 |
 |
 |
 |

© Nature
Publishing
Group
2006 |
|  |
Neutron-induced radioactivityIn September 1934,
Leo Szilard and T. H. Chalmers let gamma rays fall onto a beryllium target, noting
that emissions from the target induced radioactivity in iodine. "We conclude,"
they wrote, "that neutrons are liberated from beryllium by gamma rays."
Two months later, A. Brasch and colleagues, including Szilard and Chalmers, reported
a similar effect using X-rays rather than gamma rays. More ominously, the existence
of neutron-induced radioactivity also suggested the possibility of neutron chain-reactions
using the neutrons emitted by radioactive elements to induce radioactivity, and
liberate further neutrons, from other nuclei. The first demonstration came four
years later, following the discovery of nuclear fission in uranium (see looking
back: "Breaking up is easy nuclear fission discovered").
Nature 134, 494495; 880 (1934) | click
here for a PDF version (313 K) | | Detection
of Neutrons Liberated from Beryllium by Gamma Rays: a New Technique for Inducing
RadioactivityWe have observed that a radiation emitted from beryllium
under the influence of radium gamma rays excites induced radioactivity in iodine,
and we conclude that neutrons are liberated from beryllium by gamma rays. Chadwick
and Goldhaber were the first to observe a nuclear disintegration due to the action
of gamma rays. In their pioneer experiment1, they
used a small ionisation chamber filled with heavy hydrogen and observed that protons
were ejected from the heavy hydrogen under the influence of gamma rays from thorium
C. Their method can be used for the detection of the gamma ray disintegrations
of other elements, as such a disintegration would generally be accompanied by
the ejection of charged nuclei which their method is designed to detect.
On the other hand, apart from the unique case of heavy hydrogen, their method
does not appear to give direct evidence on neutron radiations, which may
in certain cases accompany gamma ray disintegrations. It appeared to us
of interest to search for such neutron radiations, and we thought that the Fermi
effect might conveniently be used as an indicator of their presence. For certain
reasons, we chose to use as indicators elements which, like iodine, are transmuted
in the Fermi effect into their own radioactive isotopes. In order to make
our test more sensitive, we applied in this work the new principle of isotopic
separation which we recently described2. In the
present experiment we have used iodine as indicator, and separated radio-iodine
from the bombarded iodine. In one experiment we surrounded 150 mgm of radium
(in sealed containers of 1.0 mm platinum filtration) with 25 gm of beryllium,
which was further surrounded by 100 c.c. ethyl iodide. The silver iodide precipitate
obtained after irradiation from the ethyl iodide showed an activity decaying with
a half period of 30 minutes. In spite of the inefficient geometrical arrangement
of the beryllium in this experiment, we obtained from the active precipitate 200
impulses of the Geiger-Müller beta ray counter per minute. In the control
experiment omitting the beryllium, we obtained less than 12 impulses per minute.
The effect observed is sufficiently strong to be easily detected without separating
chemically the radioactive element. Our observations show that it will be
possible to make experiments on induced radioactivity by using the gamma rays
of sealed radium containers, which are available in many hospitals for therapeutic
purposes. Further, it will be possible to have very much stronger sources of neutrons
and to produce thereby larger quantities of radioactive elements by using X-rays
from high-voltage electron tubes. LEO SZILABD.
T. A. CHALMERS. Physics Department, Medical College,
St. Bartholomew's Hospital, London, E.C.1. Sept. 17. - Nature
134, 237 Aug. 18, 1934.
- Nature
134, 462 Sept. 22, 1934.
Liberation of Neutrons
from Beryllium by X-Rays: Radioactivity Induced by Means of Electron Tubes IT
has been recently reported1 that neutrons are
liberated from beryllium by g-rays of radium and that
these are able to induce radioactivity in iodine. Following up this work, we have
attempted to liberate neutrons from beryllium by means of hard X-rays, produced
by high-voltage electron tubes. An electron tube, which could conveniently be
operated by a high-voltage impulse generator at several million volts2,
is at present in use in the High Tension Laboratory of the A.E.G. in Berlin, and
has served in the present experiment for the production of X-rays. X-rays
from a tungsten anticathode generated at a voltage above 1.5 × 106
v. were allowed to fall on beryllium. An organic bromine compound (bromoform)
was exposed to the radiation of the beryllium and this compound was then sent
by air from Berlin to London. Here, at St. Bartholomew's Hospital, after an isotopic
separation3 of the radio-bromine from the ordinary
bromine, a weak activity decaying with the six-hour period of radio-bromine was
observed. Afterwards, at a higher voltage, but still below 2 × 106
v., very much stronger activities were induced in bromine and were observed both
in Berlin and London. Strong activities were observed in Berlin both in bromine
and iodine (30 minutes half-life period) in co-operation with K. Philipp and O.
Erbacher of the Kaiser Wilhelm Institute for Chemistry, the activity and its decay
being easily measured by means of an electroscope. Recently, Fermi, Amaldi, Pontecorvo,
Rasetti and Segrè discovered4 that by surrounding
the irradiated material with substances containing hydrogen the efficiency of
activation of certain elements by neutron bombardment is greatly increased. Use
was made of this effect in these experiments. A very sharp increase of the
induced activity with increasing voltage is to be expected if there is a more
or less sharply defined upper limit of the wave-length at which the liberation
of neutrons from beryllium begins. If there is such a critical wave-length, and
if the voltage applied to the tube only slightly exceeds the corresponding critical
voltage, a small fraction only of the total X-ray energy will be present in the
form of radiation of sufficiently short wave-length; this fraction will then increase
sharply with the excess voltage. We wish to thank Prof. L. Meitner for her
kind assistance in the Berlin experiments. A. BRASCH.
F. LANGE. A. WALY. Berlin. T.
E. BANKS. T. A. CHALMERS. LEO
SZILARD. F. L. HOPWOOD. Medical
College, St. Bartholomew's Hospital, London, E.C.1. Nov. 26.
- Szilard and Chalmers, Nature 134, 494 Sept.
29, 1934.
- Brasch and Lange, Z. Phy., 70,
H. 1/2.
- Szilard and Chalmers, Nature 134,
462 Sept. 22, 1934.
- Fermi, Amaldi, Pontecorvo, Rasetti
and Segrè, La Ricerca Scientifica, 2, Nos. 78.
|
return to
looking back index page | |