References
R. H. Dalitz: inLes Houches Lectures (New York, 1965).
O. W. Greenberg:Phys. Rev. Lett.,13, 598 (1964);R. H. Dalitz: inProceedings of the Conference on Particle Physics, University of Hawai, 1967 (Honolulu, 1968).
D. Faiman andA. Hendry:Phys. Rev.,173, 1720 (1968);180, 1572 (1969).
L. A. Copley, G. Karl andE. Obrik:Phys. Lett.,29 B, 117 (1969);Nucl. Phys.,13 B, 1303 (1969).
K. C. Bowler:Phys. Rev. D,1, 926 (1970).
A. M. Baldin:Nucl. Phys.,18, 310 (1966).
V. A. Petrun’kin:Žurn. Ėksp. Teor. Fiz.,40, 1148 (1961);Sov. Phys. JETP,13, 808 (1961).
See,e.g.,M. Verde: inhandbuch der Physik, edited byS. Flügge (Berlin, 1957).
A. N. Mitra andM. Ross:Phys. Rev.,158, 1630 (1967).
V. I. Goldanskii, D. A. Karpuklin, A. V. Kutsenko andV. V. Pavlovskaia:Žurn. Ėksp. Teor. Fiz.,38, 1965 (1960);Sov. Phys. JETP 11, 1223 (1960). Note that in the value quoted for α E in this reference it is included the contribution of the Dirac charge mean square radius <r 21 >. The relation with our α is (6) α E =α+(e 2〈r 31 〉/3M.
G. Breit andM. L. Rustgi:Phys. Rev.,114, 831 (1959).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Ragusa, S. The electric polarizability of the nucleon and the harmonic-oscillator symmetric quark model. Lett. Nuovo Cimento 1, 416–418 (1971). https://doi.org/10.1007/BF02785169
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02785169