Geoffrey Chew and Steven Frautschi, in 1961, will propose that mesons, when plotted with their angular momentum, against the squared of their masses, will fall into straight line trajectories. These are called Regge trajectories.
This image represents an example of a Regge trajectory. These are the families that mesons make, when, the squared of their mass is plotted against their angular momentum. These straight line trajectories will later understood be to having had arised from the massless end points of rotating relativistic strings. This also led to the conclusion that none of these strongly interacting particles were elementary.
Regge theory, although it was of interest in the 1960s, will be succeeded by quantum chromodynamics as the proper theory of the strong interaction.
Geoffrey Chew
Steven Frautschi
Tullio Regge
This school of thought, from which string theory emerged, was led by Geoffrey Chew. The theory relied on the self consistency of the S-matrix. Remember, the S-matrix is a mathematical description of the collision of particles. This S-matrix in Chew's theory obeyed a rigorous set of mathematical properties. In fact, they were so restrictive, that only one solution could be possible. This was known as the "bootstrap approach." Chew's theory was based entirely on the S-matrix, hence, it was called S-matrix theory. This is to distinguish it from the actual S-matrix itself, which is used more broadly by physicists. The S-matrix theory was a distinct framework from quantum field theory. The notion of an elementary particle is different in each of these theories. In quantum field theory, an elementary particle is fundamental. However, in the S-matrix theory, there are an infinite series of particles, hence, none can be truly fundamental. However, it should be noted that the S-matrix theory is extremely difficult to calculate with. It is hard to extract usable data from the S-matrix theory.