  The Riemann-Lanczos problem for 4-dimensional manifolds was discussed by
Bampi and Caviglia. Using exterior differential systems they showed that it was
not an involutory differential system until a suitable prolongation was made.
Here, we introduce the alternative Janet-Riquier theory and use it to consider
the Riemann-Lanczos problem in 2 and 3 dimensions. We find that in 2
dimensions, the Riemann-Lanczos problem is a differential system in involution.
It depends on one arbitrary function of 2 independent variables when no
differential gauge condition is imposed but on 2 arbitrary functions of one
independent variable when the differential gauge condition is imposed. For each
of the two possible signatures we give the general solution in both instances
to show that the occurrence of characteristic coordinates need not affect the
result. In 3 dimensions, the Riemann-Lanczos problem is not in involution as a
identity occurs. This does not prevent the existence of singular solutions. A
prolongation of this problem, where an integrability condition is added, leads
to an involutory prolonged system and thereby generates non-singular solutions
of the prolonged Riemann-Lanczos problem. We give a singular solution for the
unprolonged Riemann-Lanczos problem for the 3-dimensional reduced Goedel
spacetime.
