In 1937, John Archibald Wheeler introduced the S-matrix and this introduction was again repeated by Heisenberg in 1943. The elements of these matrices are the strengths of scattered wave and particle interactions.
Many years later, it is becoming a critical part of many modern quantum field theories. Some have always believed that it can be used to solve the problems of the strong interactions by ways of infinitesimal local descriptions of the color forces of gluons' interactions.
The fact that these gluons can never be detected indicates that the interactions can only be effective at short distances giving a theory that is purely a local gauge invariance. The gauge concept is used with the same meaning as Heisenberg's original proposal for a fundamental length in 1938.


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