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Murray Gell-Mann tells his life story at Web of Stories [permanent dead link ] Johnson, George (October 1999). Strange Beauty: Murray Gell-Mann and the Revolution in 20th Century Physics (1st ed.). Alfred A. Knopf. ISBN 978-0-679-43764-2. The Making of a Physicist: A Talk With Murray Gell-Mann Archived May 17, 2021, at the Wayback Machine
The model was independently proposed by physicists Murray Gell-Mann, [1] who dubbed them "quarks" in a concise paper, and George Zweig, [2] [3] who suggested "aces" in a longer manuscript. André Petermann also touched upon the central ideas from 1963 to 1965, without as much quantitative substantiation.
Both the American physicist Murray Gell-Mann and the Israeli physicist Yuval Ne'eman independently and simultaneously proposed the idea in 1961. [1] [2] [a] The name comes from Gell-Mann's (1961) paper and is an allusion to the Noble Eightfold Path of Buddhism. [3]
The quark model was independently proposed by physicists Murray Gell-Mann and George Zweig in 1964. [5] Quarks were introduced as parts of an ordering scheme for hadrons, and there was little evidence for their physical existence until deep inelastic scattering experiments at the Stanford Linear Accelerator Center in 1968.
When the quark model was first postulated by Murray Gell-Mann and others in the 1960s, it was to organize the states known then to be in existence in a meaningful way. As quantum chromodynamics (QCD) developed over the next decade, it became apparent that there was no reason why only three-quark and quark-antiquark combinations could exist.
Gell-Mann and George Zweig, correcting an earlier approach of Shoichi Sakata, went on to propose in 1963 that the structure of the groups could be explained by the existence of three flavors of smaller particles inside the hadrons: the quarks. Gell-Mann also briefly discussed a field theory model in which quarks interact with gluons. [12] [13]
The theorem was proved first by Gell-Mann and Low in 1951, making use of the Dyson series. [1] In 1969, Klaus Hepp provided an alternative derivation for the case where the original Hamiltonian describes free particles and the interaction is norm bounded. [2] In 1989, G. Nenciu and G. Rasche proved it using the adiabatic theorem. [3]
The physical basis behind both isospin and strangeness was only explained in 1964, when Gell-Mann [9] and George Zweig [10] [11] independently proposed the quark model, which at that time consisted only of the up, down, and strange quarks. [12] Up and down quarks were the carriers of isospin, while the strange quark carried strangeness.