  The TMD soft function can be obtained by formulating the Wilson line in terms
of auxiliary 1-dimensional fermion fields on the lattice. In this formulation,
the directional vector of the auxiliary field in Euclidean space has the form
$\tilde n = (in^0, \vec 0_\perp, n^3)$, where the time component is purely
imaginary. The components of these complex directional vectors in the Euclidean
space can be mapped directly to the rapidities of the Minkowski space soft
function. We present the results of the one-loop calculation of the Euclidean
space analog to the soft function using these complex directional vectors. As a
result, we show that the calculation is valid only when the directional vectors
obey the relation: $|r| = |n^3/n^0| > 1$, and that this result corresponds to a
computation in Minkowski space with space-like directed Wilson lines. Finally,
we show that a lattice calculable object can be constructed that has the
desired properties of the soft function.
