Eta invariants as sliceness obstructions and their relation to Casson-Gordon invariants.
Factorisation is not unique for higher dimensional knots.
Faithful linear representations of the braid groups
Families of polynomials with total Milnor number constant.
Fibered Knots and Foliations of Highly Connected Manifolds.
Fibring the complement of the Fenn-Rolfsen link.
In this note it is shown that the complement of the singular linked spheres in four dimensions defined by Fenn and Rolfsen can be fibred by tori.Also a symmetry between the two components is revealed which shows that the image provides an example of a Spanier-Whitehead duality. This provides an immediate proof that the α-invariant is non zero.
Finite Knot Modules and the Factorization of Certain Simple Knots.
Finiteness Theorems for Conjugacy Classes and Branched Covers of Knots.
Finitude du nombre des classes d'isomorphisme des structures isométriques entières.
Forme de Blanchfield et cobordisme d'entrelacs bords.
Formes hermitiennes sur les -modules
Fundamental Groups, ...-groups and Codimension two Submanifolds
Generalized Chern-Simons theory and skein relations in arbitrary dimensions
Geometric invariants of link cobordism.
Geometrically fibred two-knots.
Grothendieck Groups of Sesquilinear Forms over a Ring with Involution.
Hermitian forms on link modules.
High-dimensional knots corresponding to the fractional Fibonacci groups
We prove that the natural HNN-extensions of the fractional Fibonacci groups are the fundamental groups of high-dimensional knot complements. We also give some characterization and interpretation of these knots. In particular we show that some of them are 2-knots.
Higher dimensional simple knots and minimal Seifert surfaces.
Homogeneity of dynamically defined wild knots.
In this paper we prove that a wild knot K which is the limit set of a Kleinian group acting conformally on the unit 3-sphere, with its standard metric, is homogeneous: given two points p, q ∈ K, there exists a homeomorphism f of the sphere such that f(K) = K and f(p) = q. We also show that if the wild knot is a fibered knot then we can choose an f which preserves the fibers.