Age, Biography and Wiki
John Stewart Bell was born on 28 July, 1928 in Belfast, Northern Ireland, UK, is a Northern Irish physicist (1928–1990). Discover John Stewart Bell's Biography, Age, Height, Physical Stats, Dating/Affairs, Family and career updates. Learn How rich is he in this year and how he spends money? Also learn how he earned most of networth at the age of 62 years old?
Popular As |
John Stewart Bell |
Occupation |
N/A |
Age |
62 years old |
Zodiac Sign |
Leo |
Born |
28 July, 1928 |
Birthday |
28 July |
Birthplace |
Belfast, Northern Ireland, UK |
Date of death |
1 October, 1990 |
Died Place |
Geneva, Switzerland |
Nationality |
Ireland
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He is a member of famous with the age 62 years old group.
John Stewart Bell Height, Weight & Measurements
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Dating & Relationship status
He is currently single. He is not dating anyone. We don't have much information about He's past relationship and any previous engaged. According to our Database, He has no children.
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John Stewart Bell Net Worth
His net worth has been growing significantly in 2023-2024. So, how much is John Stewart Bell worth at the age of 62 years old? John Stewart Bell’s income source is mostly from being a successful . He is from Ireland. We have estimated John Stewart Bell's net worth, money, salary, income, and assets.
Net Worth in 2024 |
$1 Million - $5 Million |
Salary in 2024 |
Under Review |
Net Worth in 2023 |
Pending |
Salary in 2023 |
Under Review |
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Not Available |
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Timeline
John Stewart Bell FRS (28 July 1928 – 1 October 1990) was a physicist from Northern Ireland and the originator of Bell's theorem, an important theorem in quantum physics regarding hidden-variable theories.
Bell was born in Belfast, Northern Ireland.
When he was 11 years old, he decided to be a scientist, and at 16 graduated from Belfast Technical High School.
This flaw in von Neumann's proof had been previously discovered by Grete Hermann in 1935, but did not become common knowledge until after it was rediscovered by Bell.
Bell reportedly said, "The proof of von Neumann is not merely false but foolish!"
In this same work, Bell showed that a stronger effort at such a proof (based upon Gleason's theorem) also fails to eliminate the hidden-variables program.
Bell then attended the Queen's University of Belfast, where, in 1948, he obtained a bachelor's degree in experimental physics and, a year later, a bachelor's degree in mathematical physics.
In 1954, he married Mary Ross, also a physicist, whom he had met while working on accelerator physics at Malvern, UK.
Bell became a vegetarian in his teen years.
According to his wife, Bell was an atheist.
Bell's career began with the UK Atomic Energy Research Establishment, near Harwell, Oxfordshire, known as AERE or Harwell Laboratory.
He went on to complete a PhD in physics at the University of Birmingham in 1956, specialising in nuclear physics and quantum field theory.
In 1960, he moved to work for the European Organization for Nuclear Research (CERN, Conseil Européen pour la Recherche Nucléaire), in Geneva, Switzerland.
There he worked almost exclusively on theoretical particle physics and on accelerator design, but found time to pursue a major avocation, investigating the foundations of quantum theory.
In 1964, after a year's leave from CERN that he spent at Stanford University, the University of Wisconsin–Madison and Brandeis University, Bell wrote a paper entitled "On the Einstein–Podolsky–Rosen paradox".
In this work, he showed that carrying forward EPR's analysis permits one to derive the famous Bell's theorem.
The resultant inequality, derived from basic assumptions that apply to all classical situations, is violated by quantum theory.
There is some disagreement regarding what Bell's inequality—in conjunction with the EPR analysis—can be said to imply.
Bell held that not only local hidden variables, but any and all local theoretical explanations must conflict with the predictions of quantum theory: "It is known that with Bohm's example of EPR correlations, involving particles with spin, there is an irreducible nonlocality."
According to an alternative interpretation, not all local theories in general, but only local hidden-variables theories (or "local realist" theories) have shown to be incompatible with the predictions of quantum theory.
Bell's interest in hidden variables was motivated by the existence in the formalism of quantum mechanics of a "movable boundary" between the quantum system and the classical apparatus:
"A possibility is that we find exactly where the boundary lies. More plausible to me is that we will find that there is no boundary. ... The wave functions would prove to be a provisional or incomplete description of the quantum-mechanical part, of which an objective account would become possible. It is this possibility, of a homogeneous account of the world, which is for me the chief motivation of the study of the so-called 'hidden variable' possibility."
Bell was impressed that in the formulation of David Bohm's nonlocal hidden-variable theory, no such boundary is needed, and it was this which sparked his interest in the field of research.
Bell also criticized the standard formalism of quantum mechanics on the grounds of lack of physical precision:
"For the good books known to me are not much concerned with physical precision. This is clear already from their vocabulary. Here are some words which, however legitimate and necessary in application, have no place in a formulation with any pretension to physical precision: system, apparatus, environment, microscopic, macroscopic, reversible, irreversible, observable, information, measurement. ... On this list of bad words from good books, the worst of all is 'measurement'."
But if he were to thoroughly explore the viability of Bohm's theory, Bell needed to answer the challenge of the so-called impossibility proofs against hidden variables.
Bell addressed these in a paper entitled "On the Problem of Hidden Variables in Quantum Mechanics".
(Bell had actually written this paper before his paper on the EPR paradox, but it did not appear until two years later, in 1966, due to publishing delays. ) Here he showed that John von Neumann's argument does not prove the impossibility of hidden variables, as was widely claimed, due to its reliance on a physical assumption that is not valid for quantum mechanics—namely, that the probability-weighted average of the sum of observable quantities equals the sum of the average values of each of the separate observable quantities.
In 1972 an experiment was conducted that, when extrapolated to ideal detector efficiencies, showed a violation of Bell's inequality.
It was the first of many such experiments.
Bell himself concluded from these experiments that "It now seems that the non-locality is deeply rooted in quantum mechanics itself and will persist in any completion."
He was elected a Foreign Honorary Member of the American Academy of Arts and Sciences in 1987.
Also of significance during his career, Bell, together with John Bradbury Sykes, M. J. Kearsley, and W. H. Reid, translated several volumes of the ten-volume Course of Theoretical Physics of Lev Landau and Evgeny Lifshitz, making these works available to an English-speaking audience in translation, all of which remain in print.
Bell was a proponent of pilot wave theory.
In 1987, inspired by Ghirardi–Rimini–Weber theory, he also advocated collapse theories.
He said about the interpretation of quantum mechanics: "Well, you see, I don't really know. For me it's not something where I have a solution to sell!"
However, in 2010, Jeffrey Bub published an argument that Bell (and, implicitly, Hermann) had misconstrued von Neumann's proof, saying that it does not attempt to prove the absolute impossibility of hidden variables, and is actually not flawed, after all.
(Thus, it was the physics community as a whole that had misinterpreted von Neumann's proof as applying universally.) Bub provides evidence that von Neumann understood the limits of his proof, but there is no record of von Neumann attempting to correct the near universal misinterpretation which lingered for over 30 years and exists to some extent to this day.
Von Neumann's proof does not in fact apply to contextual hidden variables, as in Bohm's theory.