HOMFLY polynomial

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In the mathematical field of knot theory, the HOMFLY polynomial, sometimes called the HOMFLY-PT polynomial or the generalized Jones polynomial, is a 2-variable knot polynomial, i.e. a knot invariant in the form of a polynomial of variables m and l. It generalizes both the Alexander polynomial and the Jones polynomial both of which can be obtained by appropriate substitutions from HOMFLY. The HOMFLY polynomial is a quantum invariant.[1]

The name HOMFLY combines the initials of its co-discoverers: Hoste, Ocneanu, Millett, Freyd, Lickorish, and Yetter[2]. The addition of PT recognizes independent work carried out by Przytycki and Traczyk.

The polynomial is defined using skein relations:

P( \mathrm{unknot} ) = 1,\,
\ell P(L_+) + \ell^{-1}P(L_-) + mP(L_0)=0,\,

where L + ,L ,L0 are crossing and smoothing changes on a local region of a link diagram, as indicated in the figure.

Skein (HOMFLY).svg

The HOMFLY polynomial of a link L that is a split union of two links L1 and L2 is given by P(L) = \frac{-(l+l^{-1})}{m} P(L_1)*P(L_2).

See the page on skein relation for an example of a computation using these relations.

[edit] Other HOMFLY skein relations

This polynomial can be obtained also using other skein relations:

\alpha P(L_+) - \alpha^{-1}P(L_-) = zP(L_0),\,
xP(L_+) + yP(L_-) + zP(L_0)=0,\,

[edit] Main properties

V(t)=P(\alpha=t,z=t^{1/2}-t^{-1/2}),\,

where V(t) is the Jones polynomial.

\Delta(t)=P(\alpha=1,z=t^{1/2}-t^{-1/2}),\,

where \Delta(t)\, is the Alexander polynomial.

P(L_1 \# L_2)=P(L_1)P(L_2),\,
P_K(\ell,m)=P_{Mirror Image(K)}(\ell^{-1},m),\,

[edit] References

  1. ^ http://www.hausdorff-research-institute.uni-bonn.de/geometry-and-physics-seminars
  2. ^ Freyd, P.; Yetter, D., Hoste, J., Lickorish, W.B.R., Millett, K., and Ocneanu, A. (1985). "A New Polynomial Invariant of Knots and Links". Bulletin of the American Mathematical Society 12 (2): 239–246. doi:10.1090/S0273-0979-1985-15361-3. 
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