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78                                                         P. CASSAM-CHENAÏ








                             The fundamental representation of the generators as n x n matrices is easily obtained; the
                             matrix elements have the following expressions :
















                             is that it decomposes on            with real numbers, even when the integrals
                             are complex (case of an electromagnetic field, of a molecule whose symmetry group has
                             irreducible representations which are not realizable over real numbers...) :










                             with w  (respectively v ) one-electron (respectively two-electrons) Hermitian operator
                             and Re(x)  (respectively Im(x)) real part (respectively imaginary part) of the complex
                             number x.

                             So the genuine generators of the unitary group have original properties and do not deserve
                             to be forgotten.  It would seem weird to build the theory of angular momentum using only
                                  with no mention of   and   .  It is equally surprising that only the   appear
                             in the theory of the unitary group. In short, in the traditional approach, one builds the Lie
                             algebra of the linear group but uses only the Lie subalgebra corresponding to the unitary
                             group. A more satisfactory approach would consist in generating the Lie algebra of the
                             unitary group only, using its real generators, then to define in this algebra with Eq.(3) the
                             rising and lowering operators

                             References

                              1.  J.  Paldus, J. Chem. Phys. 61, 5321 (1974).
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