SELF AND EXTERNAL MESON FIELDS

1959 ◽  
Vol 37 (4) ◽  
pp. 515-520
Author(s):  
R. T. Sharp

Instead of a single (isotopic vector) field to describe pions, it is sometimes advantageous to introduce several such fields with identical properties except for their coupling to the sources of the field (the baryons). In this way one can formally distinguish between self pions (roughly, those which can be emitted and absorbed by the same baryon) and external pions (roughly, those which are only exchanged between baryons or emitted into or absorbed from free states). K-mesons can be treated similarly. The device, which is of general applicability, simplifies many derivations and calculations in quantum field theory. As an illustration of the method it is used to derive the Low equations for scattering of pions and K-mesons by nucleons and for associated production. A suggestion is made for treating the nucleon–nucleon interaction.

2021 ◽  
pp. 2150155
Author(s):  
A. K. Kapoor

This work is continuation of a stochastic quantization program reported earlier. In this paper, we propose a consistent scheme of doing computations directly in four dimensions using conventional quantum field theory methods.


1973 ◽  
Vol 51 (17) ◽  
pp. 1861-1868
Author(s):  
A. Z. Capri

We utilize the fact that the nonrelativistic second-quantized formalism is simply a compact way of stating the n-body problem for arbitrary n, to derive the Schrödinger equations for few-body problems. This is particularly useful for models resulting from field theories in which a field is coupled to itself via another field, as in the case of nucleon–nucleon coupling via mesons. In this latter case, one obtains an effective nonlocal, energy dependent potential which itself depends on the possible states of the system.


1961 ◽  
Vol 20 (S2) ◽  
pp. 157-220 ◽  
Author(s):  
R. Cirelli ◽  
G. Stabilini

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