John Stewart Bell
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Born28 July 1928
Belfast, Northern IrelandDied1 October 1990
Geneva, Switzerland
Summary
John Stewart Bell was an Irish mathematician who worked in quantum mechanics.
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Biography
John Bell's great achievement was that during the 1960s he was able to breathe new and exciting life into the foundations of quantum theory, a topic seemingly exhausted by the outcome of the
Bohr-
Einstein debate thirty years earlier, and ignored by virtually all those who
used quantum theory in the intervening period. Bell was able to show that discussion of such concepts as 'realism', 'determinism' and 'locality' could be sharpened into a rigorous mathematical statement, 'Bell's inequality', which is capable of experimental test. Such tests, steadily increasing in power and precision, have been carried out over the last thirty years.
Indeed, almost wholly due to Bell's pioneering efforts, the subject of quantum foundations, experimental as well as theoretical and conceptual, has became a focus of major interest for scientists from many countries, and has taught us much of fundamental importance, not just about quantum theory, but about the nature of the physical universe.
In addition, and this could scarcely have been predicted even as recently as the mid-1990s, several years after Bell's death, many of the concepts studied by Bell and those who developed his work have formed the basis of the new subject area of quantum information theory, which includes such topics as quantum computing and quantum cryptography. Attention to quantum information theory has increased enormously over the last few years, and the subject seems certain to be one of the most important growth areas of science in the twenty-first century.
John Stewart Bell's parents had both lived in the north of Ireland for several generations. His father was also named John, so John Stewart has always been called Stewart within the family. His mother, Annie, encouraged the children to concentrate on their education, which, she felt, was the key to a fulfilling and dignified life. However, of her four children - John had an elder sister, Ruby, and two younger brothers, David and Robert - only John was able to stay on at school much over fourteen. Their family was not well-off, and at this time there was no universal secondary education, and to move from a background such as that of the Bells to university was exceptionally unusual.
Bell himself was interested in books, and particularly interested in science from an early age. He was extremely successful in his first schools, Ulsterville Avenue and Fane Street, and, at the age of eleven, passed with ease his examination to move to secondary education. Unfortunately the cost of attending one of Belfast's prestigious grammar schools was prohibitive, but enough money was found for Bell to move to the Belfast Technical High School, where a full academic curriculum which qualified him for University entrance was coupled with vocational studies.
Bell then spent a year as a technician in the Physics Department at Queen's University Belfast, where the senior members of staff in the Department, Professor Karl Emeleus and Dr Robert Sloane, were exceptionally helpful, lending Bell books and allowing him to attend the first year lectures. Bell was able to enter the Department as a student in 1945. His progress was extremely successful, and he graduated with First-Class Honours in Experimental Physics in 1948. He was able to spend one more year as a student, in that year achieving a second degree, again with First-Class Honours, this time in Mathematical Physics. In Mathematical Physics, his main teacher was Professor Peter Paul Ewald, famous as one of the founders of X-ray crystallography; Ewald was a refugee from Nazi Germany.
Bell was already thinking deeply about quantum theory, not just how to use it, but its conceptual meaning. In an interview with Jeremy Bernstein, given towards the end of his life and quoted in Bernstein's book [
1], Bell reported being perplexed by the usual statement of the
Heisenberg uncertainty or indeterminacy principle (\Delta x \Delta p ≥ \hbarΔxΔp≥ℏ, where \Delta xΔx and \Delta pΔp are the uncertainties or indeterminacies, depending on one's philosophical position, in position and momentum respectively, and ℏ is the (reduced)
Planck's constant).
It looked as if you could take this size and then the position is well defined, or that size and then the momentum is well defined. It sounded as if you were just free to make it what you wished. It was only slowly that I realized that it's not a question of what you wish. It's really a question of what apparatus has produced this situation. But for me it was a bit of a fight to get through to that. It was not very clearly set out in the books and courses that were available to me. I remember arguing with one of my professors, a Doctor Sloane, about that. I was getting very heated and accusing him, more or less, of dishonesty. He was getting very heated too and said, 'You're going too far'.
At the conclusion of his undergraduate studies Bell would have liked to work for a PhD. He would also have liked to study the conceptual basis of quantum theory more thoroughly. Economic considerations, though, meant that he had to forget about quantum theory, at least for the moment, and get a job, and in 1949 he joined the UK Atomic Research Establishment at Harwell, though he soon moved to the accelerator design group at Malvern.
It was here that he met his future wife, Mary Ross, who came with degrees in mathematics and physics from Scotland. They married in 1954 and had a long and successful marriage. Mary was to stay in accelerator design through her career; towards the end of John's life he returned to problems in accelerator design and he and Mary wrote some papers jointly. Through his career he gained much from discussions with Mary, and when, in 1987, his papers on quantum theory were collected [
21], he included the following words:
I here renew very especially my warm thanks to Mary Bell. When I look through these papers again I see her everywhere.
Accelerator design was, of course, a relatively new field, and Bell's work at Malvern consisted of tracing the paths of charged particles through accelerators. In these days before computers, this required a rigorous understanding of electromagnetism, and the insight and judgment to make the necessary mathematical simplifications required to make the problem tractable on a mechanical calculator, while retaining the essential features of the physics. Bell's work was masterly.
In 1951 Bell was offered a year's leave of absence to work with Rudolf Peierls, Professor of Physics at Birmingham University. During his time in Birmingham, Bell did work of great importance, producing his version of the celebrated CPT theorem of quantum field theory. This theorem showed that under the combined action of three operators on a physical event: PP, the parity operator, which performed a reflection; CC, the charge conjugation operator, which replaced particles by anti-particles; and TT, which performed a time reversal, the result would be another possible physical event.
Unfortunately Gerhard Lüders and
Wolfgang Pauli proved the same theorem a little ahead of Bell, and they received all the credit.
However, Bell added another piece of work and gained a PhD in 1956. He also gained the highly valuable support of Peierls, and when he returned from Birmingham he went to Harwell to join a new group set up to work on theoretical elementary particle physics. He remained at Harwell till 1960, but he and Mary gradually became concerned that Harwell was moving away from fundamental work to more applied areas of physics, and they both moved to CERN, the Centre for European Nuclear Research in Geneva. Here they spent the remainder of their careers.
Bell published around 80 papers in the area of high-energy physics and quantum field theory. Some were fairly closely related to experimental physics programmes at CERN, but most were in general theoretical areas.
The most important work was that of 1969 leading to the Adler-Bell-Jackiw (ABJ) anomaly in quantum field theory. This resulted from joint work of Bell and Ronan Jackiw, which was then clarified by Stephen Adler. They showed that the standard current algebra model contained an ambiguity. Quantisation led to a symmetry breaking of the model. This work solved an outstanding problem in particle physics; theory appeared to predict that the neutral pion could not decay into two photons, but experimentally the decay took place, as explained by ABJ. Over the subsequent thirty years, the study of such anomalies became important in many areas of particle physics. Reinhold Bertlmann, who himself did important work with Bell, has written a book titled
Anomalies in Quantum Field Theory [
10], and the two surviving members of ABJ, Adler and Jackiw shared the 1988
Dirac Medal of the International Centre for Theoretical Physics in Trieste for their work.
While particle physics and quantum field theory was the work Bell was paid to do, and he made excellent contributions, his great love was for quantum theory, and it is for his work here that he will be remembered. As we have seen, he was concerned about the fundamental meaning of the theory from the time he as an undergraduate, and many of his important arguments had their basis at that time.
The conceptual problems may be outlined using the spin-\large\frac{1}{2}\normalsize21 system. We may say that when the state-vector is \alpha_{+}α+ or \alpha_{-}α− respectively, s_{z}sz is equal to \large\frac{1}{2}\normalsize \hbar21ℏ and -\large\frac{1}{2}\normalsize \hbar−21ℏ respectively, but, if one restricts oneself to the
Schrödinger equation, s_{x}sx and s_{y}sy just do not have values. All one can say is that if a measurement of s_{x}sx, for example, is performed, the probabilities of the result obtained being either \large\frac{1}{2}\normalsize \hbar21ℏ or -\large\frac{1}{2}\normalsize \hbar−21ℏ are both \large\frac{1}{2}\normalsize21.
If, on the other hand, the initial state-vector has the general form of c_{+}\alpha_{+}+ c_{-}\alpha_{-}c+α++c−α−, then all we can say is that in a measurement of s_{z}sz, the probability of obtaining the value of \large\frac{1}{2}\normalsize \hbar21ℏ is |c_{+}^{2} |∣c+2∣, and that of obtaining the value of -\large\frac{1}{2}\normalsize \hbar−21ℏ is |c_{-}^{2} |∣c−2∣. Before any measurement, s_{z}sz just does not have a value.
These statements contradict two of our basic notions. We are rejecting
realism, which tells us that a quantity has a value, to put things more grandly -- the physical world has an existence, independent of the actions of any observer.
Einstein was particularly disturbed by this abandonment of realism -- he insisted in the existence of an
observer-free realm. We are also rejecting
determinism, the belief that, if we have a complete knowledge of the state of the system, we can predict exactly how it will behave. In this case, we know the state-vector of the system, but cannot predict the result of measuring s_{z}sz.
It is clear that we could try to recover realism and determinism if we allowed the view that the
Schrödinger equation, and the wave-function or state-vector, might not contain all the information that is available about the system. There might be other quantities giving extra information --
hidden variables. As a simple example, the state-vector above might apply to an ensemble of many systems, but in addition a hidden variable for each system might say what the actual value of s_{z}sz might be. Realism and determinism would both be restored; s_{z}sz would have a value at all times, and, with full knowledge of the state of the system, including the value of the hidden variable, we can predict the result of the measurement of s_{z}sz .
A complete theory of hidden variables must actually be more complicated than this -- we must remember that we wish to predict the results of measuring not just s_{z}sz, but also s_{x}sx and s_{y}sy, and any other component of ss. Nevertheless it would appear natural that the possibility of supplementing the
Schrödinger equation with hidden variables would have been taken seriously. In fact, though,
Niels Bohr and
Werner Heisenberg were convinced that one should not aim at realism. They were therefore pleased when
John von Neumann proved a theorem claiming to show rigorously that it is impossible to add hidden variables to the structure of quantum theory. This was to be very generally accepted for over thirty years.
Bohr put forward his (perhaps rather obscure) framework of
complementarity, which attempted to explain why one should not expect to measure s_{x}sx and s_{y}sy (or xx and pp) simultaneously. This was his
Copenhagen interpretation of quantum theory.
Einstein however rejected this, and aimed to restore realism. Physicists almost unanimously favoured
Bohr.
Einstein's strongest argument, though this did not become very generally apparent for several decades lay in the famous
Einstein-Podolsky-Rosen (EPR) argument of 1935, constructed by
Einstein with the assistance of his two younger co-workers, Boris Podolsky and Nathan Rosen. Here, as is usually done, we discuss a simpler version of the argument, thought up somewhat later by David Bohm.
Two spin-\large\frac{1}{2}\normalsize21 particles are considered; they are formed from the decay of a spin-\large\frac{1}{2}\normalsize21 particle, and they move outwards from this decay in opposite directions. The combined state-vector may be written as (\large\frac{1}{√2}\normalsize )(\alpha_{1-}\alpha_{2+} - \alpha_{1-} \alpha_{2+})(√21)(α1−α2+−α1−α2+), where the \alpha_{1}sα1s and \alpha_{2}sα2s for particles 1 and 2 are related to the \alpha sαs above. This state-vector has a strange form. The two particles do not appear in it independently; rather either state of particle 1 is correlated with a particular state of particle 2. The state-vector is said to be
entangled.
Now imagine measuring s_{1}zs1z. If we get +\large\frac{1}{2}\normalsize v+21v, we know that an immediate measurement of s_{2}zs2z is bound to yield -\large\frac{1}{2}\normalsize \hbar−21ℏ, and vice-versa, although, at least according to Copenhagen, before any measurement, no component of either spin has a particular value.
The result of this argument is that at least one of three statements must be true:
(1) The particles must be exchanging information instantaneously i.e. faster than light;
(2) There are hidden variables, so the results of the experiments are pre-ordained; or
(3) Quantum theory is not exactly true in these rather special experiments.
The first possibility may be described as the renunciation of the principle of
locality, whereby signals cannot be passed from one particle to another faster than the speed of light. This suggestion was anathema to
Einstein. He therefore concluded that if quantum theory was correct, so one ruled out possibility (3), then (2) must be true. In
Einstein's terms, quantum theory was not
complete but needed to be supplemented by hidden variables.
Bell regarded himself as a follower of
Einstein. He told Bernstein [
1]:
I felt that
Einstein's intellectual superiority over
Bohr, in this instance, was enormous; a vast gulf between the man who saw clearly what was needed, and the obscurantist.
Bell thus supported realism in the form of hidden variables. He was delighted by the creation in 1952 by David Bohm of a version of quantum theory which included hidden variables, seemingly in defiance of
von Neumann's result. Bell wrote [
21]:
In 1952 I saw the impossible done.
In 1964, Bell made his own great contributions to quantum theory. First he constructed his own hidden variable account of a measurement of any component of spin. This had the advantage of being much simpler that Bohm's work, and thus much more difficult just to ignore. He then went much further than Bohm by demonstrating quite clearly exactly what was wrong with
von Neumann's argument.
Von Neumann had illegitimately extended to his putative hidden variables a result from the variables of quantum theory that the expectation value of A + BA+B is equal to the sum of the expectation values of AA and of BB. (The expectation value of a variable is the mean of the possible experimental results weighted by their probability of occurrence.) Once this mistake was realized, it was clear that hidden variables theories of quantum theory were possible.
However Bell then demonstrated certain unwelcome properties that hidden variable theories must have. Most importantly they must be non-local. He demonstrated this by extending the EPR argument, allowing measurements in each wing of the apparatus of any component of spin, not just s_{z}sz. He found that, even when hidden variables are allowed, in some cases the result obtained in one wing must depend on which component of spin is measured in the other; this violates locality. The solution to the EPR problem that
Einstein would have liked, rejecting (1) but retaining (2) was illegitimate. Even if one retained (2), as long as one maintained (3) one had also to retain (1).
Bell had showed rigorously that one could not have local realistic theories of quantum theory. Henry Stapp called this result [
18]:
the most profound discovery of science.
The other property of hidden variables that Bell demonstrated was that they must be
contextual. Except in the simplest cases, the result you obtained when measuring a variable must depend on which other quantities are measured simultaneously. Thus hidden variables cannot be thought of as saying what value a quantity 'has', only what value we will get if we measure it.
Let us return to the locality issue. So it has been assumed that quantum theory is exactly true, but of course this can never be known. John Clauser, Richard Holt, Michael Horne and Abner Shimony adapted Bell's work to give a direct experimental test of local realism. Thus was the famous CHHS-Bell inequality [
19], often just called the Bell inequality. In EPR-type experiments, this inequality is obeyed by local hidden variables, but may be violated by other theories, including quantum theory.
Bell has reached what has been called
experimental philosophy; results of considerable philosophical importance may be obtained from experiment. The Bell inequalities have been tested over nearly thirty years with increasing sophistication, the experimental tests actually using photons with entangled polarisations, which are mathematically equivalent to the entangled spins discussed above. While many scientists have been involved, a selection of the most important would include Clauser, Alain Aspect and Anton Zeilinger.
While at least one loophole still remains to be closed [in August 2002], it seems virtually certain that local realism is violated, and that quantum theory can predict the results of all the experiments.
For the rest of his life, Bell continued to criticize the usual theories of measurement in quantum theory. Gradually it became at least a little more acceptable to question
Bohr and
von Neumann, and study of the meaning of quantum theory has become a respectable activity.
Bell himself became a Fellow of the
Royal Society as early as 1972, but it was much later before he obtained the awards he deserved. In the last few years of his life he was awarded the Hughes Medal of the
Royal Society, the
Dirac Medal of the Institute of Physics, and the Heineman Prize of the American Physical Society. Within a fortnight in July 1988 he received honorary degrees from both Queen's and Trinity College Dublin. He was nominated for a Nobel Prize; if he had lived ten years longer he would certainly have received it.
This was not to be. John Bell died suddenly from a stroke on 1st October 1990. Since that date, the amount of interest in his work, and in its application to quantum information theory has been steadily increasing.
https://mathshistory.st-andrews.ac.uk/Biographies/Bell_John/
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