Topology in Molecular Biology

84 L.H. Kauffman and S. Lambropoulou

: or

: or

++

Fig. 5.13.Crossing signs and curls

in Fig. 5.13. Note that the type of a curl does not depend on the orientation
we choose. The small arcs on the right-hand side of these formulas indicate
the removal of the curl from the corresponding diagram.
The bracket is invariant under regular isotopy and can be normalized to
an invariant of ambient isotopy by the definition

fK(A)=(−A^3 )−w(K)〈K〉(A),

where we chose an orientation forK, and wherew(K) is the sum of the
crossing signs of the oriented linkK.w(K) is called thewritheofK.The
convention for crossing signs is shown in Fig. 5.13.
By a change of variables one obtains the original Jones polynomial,VK(t),
for oriented knots and links from the normalized bracket:

VK(t)=fK(t−^1 /^4 ).
The bracket model for the Jones polynomial is quite useful both theoreti-
cally and in terms of practical computations. One of the neatest applications
is to simply computefK(A) for the trefoil knotTand determine thatfT(A)
is not equal tofT(A−^1 )=f−T(A).This shows that the trefoil is not ambient
isotopic to its mirror image, a fact that is quite tricky to prove by classical
methods.
For two-tangles, we do smoothings on the tangle diagram until there are
no crossings left. As a result,a state of a two-tangleconsists in a collection
of loops in the tangle box, plus simple arcs that connect the tangle ends. The
loops evaluate to powers ofδ, and what is left is either the tangle [0] or the
tangle [∞], since [0] and [∞] are the only ways to connect the tangle inputs
and outputs without introducing any crossings in the diagram. In analogy to