An axiomatic deduction of the pauli spinor theory

1977 ◽  
Vol 16 (4) ◽  
pp. 249-257 ◽  
Author(s):  
H. M. Schwartz
Keyword(s):  

2021 ◽  
Vol 1820 (1) ◽  
pp. 012168
Author(s):  
Guangqi Ying ◽  
Genbao Zhang ◽  
Yan Ran ◽  
Zongyi Mu
Keyword(s):  


1975 ◽  
Vol 30 (5) ◽  
pp. 656-671
Author(s):  
W. Bauhoff

AbstractThe mass eigenvalue equation for mesons in nonlinear spinor theory is derived by functional methods. In second order it leads to a spinorial Bethe-Salpeter equation. This is solved by a variational method with high precision for arbitrary angular momentum. The results for scalar mesons show a shift of the first order results, obtained earlier. The agreement with experiment is improved thereby. An excited state corresponding to the η' is found. A calculation of a Regge trajectory is included,too.



1971 ◽  
Vol 4 (2) ◽  
pp. 404-420 ◽  
Author(s):  
H. Saller


1967 ◽  
Vol 70 ◽  
pp. 505-523
Author(s):  
D.C. van Drooge
Keyword(s):  


1974 ◽  
Vol 29 (7) ◽  
pp. 981-990
Author(s):  
K. Dammeier

A pole regularized nonlinear spinor theory may be a suitable test object to compare scattering calculations of Stumpf's functional quantum theory with LSZ-results. To apply the LSZ-technique in this theory, a dressing of the occurring massless Green's function is necessary. It is shown which special approximations allow for this dressing. The renormalized nucleon-nucleon coupling constant yields the right order of magnitude for the elastic nucleon cross section.



1972 ◽  
Vol 27 (7) ◽  
pp. 1058-1072
Author(s):  
H Stumpf

Abstract Nonlinear spinor theory contains unobservable field operators which cannot be identified with free field operators. Therefore for the comparson with experiment a theory of observables for nonlinear spinor fields is required. This theory is developed for global observables by means of a map into functional space, and leads to a functional quantum theory of nonlinear spinor fields



1961 ◽  
Vol 16 (3) ◽  
pp. 225-227
Author(s):  

The contraction function 〈0 | T ψα(x) ψ̅β(x′) |0〉 occurring in the nonlinear spinor-theory of HEISENBERG has been approximated by assuming that the density function ρ (ζ) contains a normal particle state at ζ=ϰ2 and α dipoleghost at ζ= m2. This assumption is slightly more general than that in the original paper where the mass of the dipoleghost was taken as ζ=0. The intention of the present calculation was to see whether the approximaion could be improved in this way and whether a certain inconsistency mentioned in the earlier paper would disappear. The nucleon massvalue xN l is calculated in the lowest approximation of the new TAMM-DANCOFF method. It is shown that only for m2/ϰ2 less than about 0.05 real values of ϰN l are obtained, i. e. the dipoleghost has to be assumed at zero mass or very near to it. The inconsistency of the method mentioned in earlier work still persists.



1968 ◽  
Vol 54 (3) ◽  
pp. 639-694 ◽  
Author(s):  
H. P. Dürr ◽  
F. Wagner


1974 ◽  
Vol 23 (1) ◽  
pp. 1-32 ◽  
Author(s):  
H. P. Dürr ◽  
P. du T. van der Merwe


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