Presentation Speech by Professor E. Hulthén, member of the Nobel Committee for Physics
Your Majesty, Your Royal Highnesses, Ladies
and Gentlemen.
For the man in the street I suppose the compass needle is the
most familiar magnetic instrument. But when and where the compass
was first used is a much-debated question, where we grope between
Chinese records from the year 2,600 B.C. and ship's logs made by
the Norsemen in their Icelandic voyages in the 12th and 13th
centuries. It is typical of all such records, whether of
gunpowder or the compass, that they refer to inventions that had
long been in use. The very idea of invention, of having been the
first, had doubtless not the same significance formerly that it
has today. As a matter of fact, the scientific study of magnetism
in the sense in which we understand it, was begun only with the
publication in London of Gilbert's work De Magnete in the year
1,600 A.D. The subsequent investigation and classification of
magnetic substances led to their division into three categories:
the ferromagnetics or strong magnetics such as iron, cobalt and
nickel; the paramagnetic or weak magnetics, including chiefly
crystals and fluids; and finally the diamagnetics, with their
magnetic repulsion, a property intrinsic in all substances. A
compass needle made of a diamagnetic substance turns at right
angles to the magnetic lines of force, and thus comes to point in
an east-westerly direction. Fortunately, diamagnetism is too weak
to cause shipwreck in this way. This wealth of magnetic is today
joined by a fourth category, the nuclear magnetism deriving from
the atomic nucleus.
The magnetic field radiating from the infinitesimally tiny atomic
nucleus is so feeble that its existence was still scarcely more
than divined only fifteen or twenty years ago. Thus when Bloch
and Purcell, this year's Nobel Prize winners in Physics, are able
to register nuclear magnetism with a precision exceeding almost
all other measurements in physics, one supposes that this must be
thanks to the use of special methods and accessories. But what
interest or useful purpose may conceivably be served by such
subtleties?
If we consider the methods that have been employed, we soon
recognize the idea that runs through all more advanced
measurements of a body's magnetic moments. Thus the celebrated
German mathematician and physicist, Karl Friedrich Gauss,
determined in 1836 the magnetic moment of thc compass needle in
relation to its moment of inertia, simply by observing the
oscillations of the needle in a magnetic field of known
strength.
Now the electrons or the atomic nucleus do not, it is true,
behave in quite the same way as the compass needle in the
magnetic field, but rather in the manner of the top, the
gyroscope, which spins and precesses about the perpendicular. But
the electronic and nuclear spins are just as characteristic for
these particles as are their electric charge and mass (the atomic
weights), so that the deep import of a determination of their
gyromagnetic indices becomes immediately obvious.
Now what possibilities exist for the observation and measurement
of the frequencies of the electrons and the atomic nucleus in the
magnetic field? This is where the new phase in the development
comes in. In this connection I need only remind you of the
resonance between our radio apparatuses and radio waves. The
comparison is actually quite justified, as the electronic and
atomic nuclear frequencies in the magnetic field fall precisely
within the region for the short-wave radio with wavelengths
varying between some tens of meters and the centimeterwaves
employed in radar technique.
These atomic frequencies in the magnetic field are so
characteristic for each element and its isotopes that they are
more undisturbed and regular than the balance-wheel, pendulum and
vibrating quartz-crystal in our modern chronometers.
The method for the determination of the nuclear magnetic moment
through resonance with radio waves has long been well-known, and
was rewarded by the Academy of Sciences with the Nobel Prize for
the year 1944 to Rabi. It was
with similar methods that the paramagnetism of crystals deriving
from the electronic spin was investigated by Gorter in
Leiden.
Rabi carried out his investigations on nuclear magnetic moments
according to the molecular-ray method, an artificial method which
has, certainly, the inestimable advantage that the investigated
substance is in a state of very high rarefaction, though at the
same time this limits its application. The methods of Purcell and
Bloch imply a great simplification and generalization in this
respect, which enables their application to solid, liquid and
gaseous substances. This brings us to the useful purposes which
may be served. Since each kind of atom and its isotopes have a
sharply defined and characteristic nuclear frequency, we can in
any object placed between the poles of an electromagnet seek out
and examine with radio waves all the various kinds of atom and
isotopes present in the object in question, and, which is the
essential point, this without in any perceptible way
affecting the same, its form, crystalline structure, etc. This
form of analysis in situ is therefore probably not
parallelled in any other known methods of analysis. Its
extraordinary sensitiveness also makes it particularly
well-adapted as a micro-method in many scientific and technical
fields.
Professor Purcell. As far I have been able
to follow your activities since you stopped working at the great
Radiation Laboratory at M.I.T. at the end of the War, and up to your
development of the excellent method of nuclear resonance
absorption for which you have been awarded your Nobel Prize,
you have happily realized man's old dream of beating the sword
into a ploughshare. Your wide experience in electronics and the
deep interest you early showed in paramagnetic phenomena may thus
conceivably have contributed to the invention of your method,
which through its extraordinary sensitiveness gives us a deep
insight into the constitution of crystals and fluids, and the
interactions, so-called relaxations, between the tiniest
particles of matter.
In part with this method, and in part without it, you and your
collaborators have made a number of important discoveries, among
which I would like particulary to stress the three
following:
Your method for studying nuclear magnetic resonance in weak
magnetic field produced according to the solenoid method, which
is of great value for the absolute determination of nuclear
magnetic moments.
In the very interesting experiment which you performed together
with Dr. Pound, you have produced with paramagnetic resonance the
rather unique situation in which the state of the atomic nucleus
corresponds to negative temperatures in the absolute-temperature
scale.
Finally, as a quite spectacular discovery I may mention your
observation with Dr. Ewen in 1951 of a line in the galactic
radiospectrum caused by atomic hydrogen, an important
contribution to radioastronomy.
Please accept our congratulations, and receive your Nobel Prize
from the hands of His Majesty.
Professor Bloch. It would be difficult in
the few minutes at my disposal to try to give the main features
of the nuclear induction method for which you have been awarded
your Nobel Prize. It would be still more difficult for me to give
an exhaustive account of the ways that led you to this
invention.
You began your career as a theoretical physicist, well-known for
your fundamental contributions to the theory of metals.
When, quite unexpectedly, you went over to experimental research,
this must have been, I feel, with deliberation and assurance. For
you had in your kitbag a tool of extraordinary value, the method
for the magnetic polarization of a beam of neutrons. The
inestimable value of possessing a good idea, of indefatigably
testing and perfecting it, is best illustrated by your
precision-measurements of the magnetic moment of the neutron, one
of the most difficult and at the same time most important tasks
in nuclear physics.
But ideas give birth to new ideas, and it was, as I understand,
in this way that you hit upon the excellent notion of eliminating
the difficult absolute determination of the magnetic field by a
direct measurement of the neutron moment in units of the proton
cycle (the nuclear magneton). According to your own account it
was this solution which finally led you to the nuclear induction
method.
In congratulating you I now beg you to receive your Nobel Prize
from the hands of His Majesty.
From Nobel Lectures, Physics 1942-1962, Elsevier Publishing Company, Amsterdam, 1964
Copyright © The Nobel Foundation 1952