Abstract
The basic ideas and methods of the quark model of the elementary particles, and the main results of the model, including the new applications to high energy scattering are summarized and partly discussed in detail. Also the quark models of weak interactions are briefly commented.
Резюме
Излагаются основные идеи и методы кварковой модели элементарных частиц. Дается обзор, и частью подробное обсуждение главных резльтатов, включая новое применение модели к рассеянию при высоких энергиях. Кратко рассмотрены также кварковые модели слабых взаимодействий.
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References and notes
E. Fermi andC. N. Yang, Phys. Rev.,76, 1739, 1949.
S. Sakata, Progr. Theoret. Phys.,16, 686, 1956.
See, for example, lectures byChew inM. Jacob andG. F. Chew, “Strong-Interaction Physics”, W. A. Benjamin, Inc., 1964.
M. Gell-Mann, California Institute of Technology, Synchrotron Laboratory Report CTSL-20 1961, unpublished.
Y. Ne’eman, Nucl. Phys.,26, 222, 1961.
V. E. Barnes et al., Phys. Rev. Letters12, 204, 1964.
M. Gell-Mann, Phys. Letters,8, 214, 1964.
G. Zweig, “An SU 3 Model for Strong-Interaction Symmetry and its Breaking”, CERN preprints No. TH. 401 Jan. 1964, and TH. 412 Feb. 1964.
B. Sakita, Phys. Rev.,136, B226, 1964. —F. Gursey andL. A. Radicati, Phys. Rev. Letters,13, 173, 1964.
M. A. B. Bég, B. W. Lee andA. Pais, Phys. Rev. Letters,13, 514, 1966.
See, for example,H. J. Lipkin andS. Meshkov, “Spin Independence,W-Spin, Parity, andSU(6) Symmetry”, to be published in Phys. Rev.
S. L. Glashow andR. H. Socolow, Phys. Rev. Letters,15, 329, 1965, and further references given there.
For discussion, seeS. Meshkov, talk at the Coral Gables Conference, January 1966, andL. Maiani andG. Preparata, Nuovo Cimento,40, A654, 1966.
P. Federman, H. R. Rubinstein andI. Talmi, “Dynamical Derivation of Baryon Masses in the Quark Model”, to be published.
H. R. Rubinstein, “A Dynamical Quark Model for Hadrons”, to be published. This result was also obtained byI. Talmi (private communication).
The values of theSU(6) contributions have been listed byH. Harari andM. A. Rashid, Phys. Rev.,143, 1354, 1966.
H. J. Lipkin andF. Scheck, Phys. Rev. Letters,16, 71, 1966.
E. M. Levin andL. L. Frankfurt, Zhur Eksp. i Theoret. Fiz.,2, 105, 1965. English translation Soviet Phys. — JETP Letters2, 65, 1965.
For investigations at non-zero momentum transfer, seeJ. J. J. Kokkedee andL. van Hove, Nuovo Cimento42, 711, 1966, andJ. J. J. Kokkede “Quark Model and Relations between High Energy Scattering Amplitudes”, CERN preprint TH. 669.
W. Galbraith et al., Phys. Rev.,138, B913, 1965.
I am indebted for this arguments toJ. J. J. Kokkedee andL. Van Hove (private communication).
H. J. Lipkin, “Quark Models and High-Energy Scattering”, to be published.
K. Johnson andS. B. Treiman, Phys. Rev. Letters,14, 189, 1965.
This was noticed independently byJ. J. J. Kokkedee.
C. Becchi andG. Morpurgo, Phys. Rev.,140, B687, 1965.
H. R. Rubinstein, to be published.
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Socolow, R.H. Recent results from the quark model. Acta Physica 22, 129–149 (1967). https://doi.org/10.1007/BF03159468
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DOI: https://doi.org/10.1007/BF03159468