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We present a new algorithm for the reduction of one-loop \emph{tensor}Feynman integrals with $n\leq 4$ external legs to \emph{scalar} Feynmanintegrals $I_n^D$ with $n=3,4$ legs in $D$ dimensions, where $D=d+2l$ withinteger $l \geq 0$ and generic dimension $d=4-2\epsilon$, thus avoiding theappearance of inverse Gram determinants $()_4$. As long as $()_4\neq 0$, theintegrals $I_{3,4}^D$ with $D>d$ may be further expressed by the usualdimensionally regularized scalar functions $I_{2,3,4}^d$. The integrals$I_{4}^D$ are known at $()_4 \equiv 0$, so that we may extend the numerics tosmall, non-vanishing $()_4$ by applying a dimensional recurrence relation. Anumerical example is worked out. Together with a recursive reduction of 6- and5-point functions, derived earlier, the calculational scheme allows astabilized reduction of $n$-point functions with $n\leq 6$ at arbitrary phasespace points. The algorithm is worked out explicitely for tensors of rank$R\leq n$.

Some variations of the reduction of one-loop Feynman tensor integrals