scholarly journals Nucleon Magnetic Moments in Ps-Ps Intermediate Coupling Meson Theory

1956 ◽  
Vol 16 (2) ◽  
pp. 95-111 ◽  
Author(s):  
Akira Kanazawa ◽  
Masao Sugawara
Keyword(s):  
Magnetic Moments ◽  
Intermediate Coupling ◽  
Meson Theory

scholarly journals On the Use of the Tomonaga Intermediate Coupling Method in Meson Theory

1950 ◽  
Vol 79 (6) ◽  
pp. 918-925 ◽  
Author(s):  
Kenneth M. Watson ◽  
Edward W. Hart
Keyword(s):  
Coupling Method ◽  
Intermediate Coupling ◽  
Meson Theory

Pairing in shell models

1955 ◽  
Vol 232 (1188) ◽  
pp. 88-104 ◽  
Keyword(s):  
Group Theory ◽  
Shell Model ◽  
Magnetic Moments ◽  
Light Nuclei ◽  
Intermediate Coupling ◽  
Nuclear Magnetic Moments ◽  
Shell Models ◽  
Decomposition Procedure ◽  
Nuclear Magnetic

An L-S pairing shell model is proposed for light nuclei (§§2( b ) and 5). Three types of shell model, that is, super multiplet theory, j-j pairing scheme and the L-S pairing scheme are compared with respect to the decomposition procedure by group theory, and also are compared in connexion with nuclear magnetic moments (§§7, 3). It is very likely that in light nuclei the L-S pairing or an intermediate coupling between the L-S pairing and j-j pairing schemes is a very good approximation.

On the Magnetic Moments of the Nucleons in Meson Theory

1949 ◽  
Vol 75 (8) ◽  
pp. 1277-1278 ◽  
Author(s):  
J. M. Luttinger
Keyword(s):  
Magnetic Moments ◽  
Meson Theory

scholarly journals Nuclear structure is governed by the fundamental laws of electromagnetism

2019 ◽  
Vol 11 ◽  
Author(s):  
L. A. Kaliambos
Keyword(s):  
Magnetic Moments ◽  
Careful Analysis ◽  
Pauli Principle ◽  
Binding Energies ◽  
Meson Theory ◽  
Charge Independence ◽  
Independence Hypothesis ◽  
Electronic Configurations ◽  
Basic Equations ◽  
Nuclear Shell

Contradicting interpretations of the nuclear force as given by two contrasted approaches like the meson theory and the quantum chromodynamics, are overcome here by reviving the basic electromagnetic laws which are applicable on the existing charged subconstituents in nucléons. On this basis, considerable charge distributions in nucleons are determined after a careful analysis of the magnetic moments and the results of the deep inelastic scattering. Basic equations derived from the distributed charges of oriented spins of nucléons give strong and short ranged forces leading exactly to the binding energies of the deuteron and other nuclei. According to these interactions, p-p and n-n systems repel and only the p-n bonds form rectangles and closely packed parallelepipeds. Such contrary forces create structures of saturation and of finite number of nucléons. They also invalidate the charge independence hypothesis and differ fundamentally from the central potential and the effects of the Pauli principle of the electronic configurations responsible for the development of the models of the Fermi gas and nuclear shell. There are two kinds of p-n bonds, which imply anisotropy, leading often to elongated shapes of vibrational and rotational modes of excitation, while the surface tension contributes to the creation of non elongated shapes of stable arrangements. Finally, for A>40 a type of shell structure provides new rules for understanding the structure of magic nuclei for N>Z and the increasing ratio N/Z with A.

scholarly journals Intermediate Coupling Meson Theory of Nuclear Forces, II

1956 ◽  
Vol 15 (2) ◽  
pp. 137-150 ◽  
Author(s):  
Yukihisa Nogami ◽  
Hiroichi Hasegawa
Keyword(s):  
Nuclear Forces ◽  
Intermediate Coupling ◽  
Meson Theory

The nucleon Green function in pseudoscalar meson theory. II

1955 ◽  
Vol 232 (1190) ◽  
pp. 377-388 ◽  
Keyword(s):  
Green Function ◽  
Pseudoscalar Meson ◽  
Preceding Paper ◽  
Functional Integral ◽  
Coupling Constants ◽  
Intermediate Coupling ◽  
Coupled Equations ◽  
Meson Theory ◽  
Coupling Approach ◽  
The Green Function

Following the formal work of the preceding paper, a method is proposed to evaluate the functional integral which has been derived for the Green function of one nucleon interacting with a pseudoscalar meson field. The method is basically that of stationary phase taken to its second approximation, and since this approximation where applicable is accurate in the limits of strong and weak coupling constants, it is assumed good in general. There are several difficulties involved in the evaluation, and as far as possible these are isolated and discussed with the aid of models each showing one difficulty alone. Combining these separate points, the evaluation of the functional integral is thereby expressed in terms of the solution of a set of coupled equations which provide a basis for a covariant intermediate coupling approach to the problem. The solution of these equations is not attempted in this paper.

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