Deforming twist-spun knots
Deforming twist-spun knots
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使扭结变形
DOI:
10.1090/s0002-9947-1979-0530058-4
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发表时间:
1979
影响因子:
1.3
通讯作者:
R. Litherland
中科院分区:
文献类型:
--
作者:
R. Litherland
In [151 Zeeman introduced the process of twist-spinning an n-knot to obtain an (n + I)-knot, and proved the remarkable theorem that a twist-spun knot is fibred. In [21 Fox described another deformation which can be applied during the spinning process, and which he called rolling. We show that, provided one combines the rolling with a twist, the resulting knot is again fibred. In fact, this result holds for a larger class of deformations, defined below. 0. Introduction. The process of spinning may be described as follows. Suppose we have a knotted arc in half 3-space R 3i, with its endpoints in R2 = aR3 . Rotating R 3 about R2 generates R', and the arc sweeps out a knotted 2-sphere. Now suppose that during the spinning process we move the arc in R 3 (keeping its endpoints fixed); provided it is returned to its original position at the end of the spinning, we again obtain a 2-sphere in R'. We call this process deform-spinning; a precise definition (in any dimension) is given in ? 1 (where for convenience we work with the one-point compactification B3 of R 3 ). The first example of deform-spinning was given by Zeeman [15]; this was the operation of twisting the knot about its axis. Subsequently, Fox [2] described another variation on spinning, called roll-spinning, and showed that this differs from twist-spinning. (Specifically, he showed that the roll-spun figure eight knot cannot be obtained by twist-spinning the figure eight.) Now, the main result of [15] is the striking theorem that any twist-spun knot is fibred. It is natural to ask whether this can be extended to rolling, or some combination of rolling and twisting. First we need a definition of rolling; in [2] Fox only gives a picture of rolling a figure eight knot, and remarks that the operation resembles "rolling a stocking". Our first observation is that in Fox's pictures points of the arc move from the right of the knot to the left. This suggests that, instead of rolling the knot down the string, we should pull the string through the knot. In other words, we should consider an isotopy of space which moves a base-point once around the knot, and is fixed away from the knot. Unfortunately, this only makes sense for a knotted circle, and we do not get a motion of the corresponding knotted arc, Received by the editors July 14, 1977. AMS (MOS) subject classifications (1970). Primary 57C45, 55A25.