Abstract
It is shown why the symmetry principle between the baryon triplet (Λnp) and lepton triplet (μ eν) suggests a two-field theory of elementary particles. One massless spinor field is used to describe the nucleons and light leptons and a second spinor field with finite bare mass the « strange » particles Λ andμ. The two-field model resembles the theories of Heisenberg and Nambu in several respects but there are also important differences which are spelled out.
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