Exact solutions of the Helmholtz equation are constructed, possessing wavef
ront dislocation lines (phase singularities) in the form of knots or links
where the wave function vanishes ('knotted nothings'). The construction pro
ceeds by making a nongeneric structure with a strength n dislocation loop t
hreaded by a strength m dislocation line, and then perturbing this. In the
resulting unfolded (stable) structure, the dislocation loop becomes an (in,
it) torus knot if in and n are coprime, and N linked rings or knots if rn
and n have a common factor N: the loop or rings are threaded by an m-strand
ed helix. In our explicit implementation, the wave is a superposition of Be
ssel beams,, accessible to experiment. Paraxially, the construction fails.