-
4
-
-
85035281780
-
-
There is space to list only a few reviews. R. L. Jaffe, in Relativistic Dynamics and Quark-Nuclear Physics, edited by M. B. Johnson and A. Picklesimer
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There is space to list only a few reviews. R. L. Jaffe, in Relativistic Dynamics and Quark-Nuclear Physics, edited by M. B. Johnson and A. Picklesimer (unpublished)
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-
-
-
14
-
-
85035298966
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-
Our notation is that a four vector (Formula presented) is defined by the plus, minus, and perpendicular components as ((Formula presented) (Formula presented)) and (Formula presented)(Formula presented)(Formula presented)(Formula presented)(Formula presented)
-
Our notation is that a four vector (Formula presented) is defined by the plus, minus, and perpendicular components as ((Formula presented) (Formula presented)) and (Formula presented)(Formula presented)(Formula presented)(Formula presented)(Formula presented)
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-
-
-
15
-
-
85035292710
-
-
The use of scalar mesons is meant as a simple representation of the two pion exchange potential which causes much of the medium range attraction between nucleons, as well as the effects of a fundamental scalar meson. Thus the pion is an important implicit part of the present Lagrangian
-
The use of scalar mesons is meant as a simple representation of the two pion exchange potential which causes much of the medium range attraction between nucleons, as well as the effects of a fundamental scalar meson. Thus the pion is an important implicit part of the present Lagrangian.
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-
-
-
16
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-
0004241061
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ANUPBZ, Report IU-NTC-96-17, nucl-th/9701058, 1997
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B. D. Serot and J. D. Walecka, Adv. Nucl. Phys. 16, 1 (1986);ANUPBZ Report IU-NTC-96-17, nucl-th/9701058, 1997.
-
(1986)
Adv. Nucl. Phys.
, vol.16
, pp. 1
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-
Serot, B.D.1
Walecka, J.D.2
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18
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-
85035307357
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7, 1147 (1973).
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(1973)
, vol.7
, pp. 1147
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-
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20
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85035291924
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7, 1780 (1974).
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(1974)
, vol.7
, pp. 1780
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-
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24
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-
85035292402
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-
The same symbol (Formula presented) is used for the nucleon field operator and for its mode functions
-
The same symbol (Formula presented) is used for the nucleon field operator and for its mode functions.
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-
-
-
29
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-
85035292485
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-
Equation (15) is essentially Eq. (5.2) of Frankfurt and Strikman, Ref. 2
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Equation (15) is essentially Eq. (5.2) of Frankfurt and Strikman, Ref. 2, with our (Formula presented) corresponding to their (Formula presented)
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-
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32
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-
0030582046
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P. A. M. Guichon, K. Saito, E. Rodionov, and A. W. Thomas, Nucl. Phys. A601, 349 (1996)
-
(1996)
Nucl. Phys.
, vol.A601
, pp. 349
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-
Guichon, P.A.M.1
Saito, K.2
Rodionov, E.3
Thomas, A.W.4
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