In an earlier paper the first author defined a non-commutative
–polynomial
for knots in 3–space, using the colored Jones function. The idea is
that the colored Jones function of a knot satisfies a non-trivial linear
–difference
equation. Said differently, the colored Jones function of a knot is annihilated by a non-zero
ideal of the Weyl algebra which is generalted (after localization) by the non-commutative
–polynomial
of a knot.
In that paper, it was conjectured that this polynomial
(which has to do with representations of the quantum group
) specializes at
to the better known
–polynomial of a knot, which
has to do with genuine
representations of the knot complement.
Computing the non-commutative
–polynomial
of a knot is a difficult task which so far has been achieved for
the two simplest knots. In the present paper, we introduce the
–polynomial of
a knot, along with its non-commutative version, and give an explicit computation for all twist
knots. In a forthcoming paper, we will use this information to compute the non-commutative
–polynomial
of twist knots. Finally, we formulate a number of conjectures relating the
, the
–polynomial
and the Alexander polynomial, all confirmed for the class of twist knots.