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            <td style="vertical-align: top;"><a href="aboutKnots.html"><small
 style="color: rgb(0, 0, 102);">Previous</small></a><br>
            </td>
            <td
 style="text-align: center; vertical-align: top; color: rgb(0, 0, 102);"><big><span
 style="font-weight: bold;">About HAP: Computing a peripheral system
for a 3-manifold<br>
            </span></big></td>
            <td style="text-align: right; vertical-align: top;"><a
 href="aboutCoverinSpaces.html"><small style="color: rgb(0, 0, 102);">next</small></a><br>
            </td>
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      <big><span style="font-weight: bold;"></span></big><br>
      </th>
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    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 255); text-align: left;">Let
K:S<sup>1</sup>--><span style="font-weight: bold;">R</span><sup>3</sup>
be a tame knot. Let TK be a solid tubular neighbourhood of the knot,
the neighbourhood being small enough to have the homotopy type of a
circle. Let M<sub>K</sub> denote the closure of the complement <span
 style="font-weight: bold;">R</span><sup>3</sup>\TK . Then M<sub>K</sub>
is a 3-manifold. By a theorem of Waldhausen [<span
 id="CITEREFWaldhausen1968" class="citation">F. Waldhausen, "On
irreducible 3-manifolds which are sufficiently large", Annals of
Mathematics. Second Series</i> <b>87</b> (1968), 56–88] the
homeomorphism type of </span>M<sub>K</sub> is completely determined by
the canonical inclusion of fundamental groups π<sub>1</sub>(δM<sub>K</sub>)
-->
π<sub>1</sub>(M<sub>K</sub>) where δM<sub>K </sub>denotes the
boundary of M<sub>K</sub> . This homomorphism is an example of a <span
 style="font-style: italic;">peripheral system</span>. By a theorem of
Gordon
and Luecke [C. Gordon and J. Luecke, "Knots are determined by their
Complements", J. Amer. Math. Soc., 2 (1989), 371–415]
the homeomorphism type of M<sub>K</sub> completely determines the
ambient isotopy type of the knot K.<br>
      <br>
As a means of illustrating some HAP functions for computing with
topological manifolds we shall compute the homomorphism π<sub>1</sub>(δM<sub>K</sub>)
-->
π<sub>1</sub>(M<sub>K</sub>) for
the T.thermophilus 1V2X protein knot illustrated on the <a
 href="aboutKnots.html#proteins">previous page</a>.<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 255);">The
following commands first read the protein knot as a pure permutahedrall
complex from a <a
 href="1V2X.pdb">pdb
file</a> .  <br>
      </td>
    </tr>
    <tr>
      <td
 style="background-color: rgb(255, 255, 204); vertical-align: top;">gap>
K:=ReadPDBfileAsPurePermutahedralComplex("1V2X.pdb");<br>
Reading chain containing 191 atoms.<br>
Pure permutahedral complex of dimension 3.<br>
      </td>
    </tr>
    <tr>
      <td
 style="background-color: rgb(255, 255, 255); vertical-align: top;">The
advantage of working with pure permutahedral complexes is that they are
always topological manifolds. (This is not the case for pure cubical
complexes.)<br>
      <br>
The following commands compute a pure permutahedral complex M
homeomorphic to the manifold M<sub>K</sub>. The complex M is a union of
4433 3-dimensional permutahedra.<br>
      </td>
    </tr>
    <tr>
      <td
 style="background-color: rgb(255, 255, 204); vertical-align: top;">gap>
K:=ZigZagContractedPureComplex(K);<br>
Pure permutahedral complex of dimension 3.<br>
      <br>
gap> K:=PurePermutahedralComplex(FrameArray(K!.binaryArray));<br>
Pure permutahedral complex of dimension 3.<br>
      <br>
gap> M:=ComplementOfPureComplex(K);<br>
Pure permutahedral complex of dimension 3.<br>
      <br>
gap> M:=ZigZagContractedPureComplex(M);<br>
Pure permutahedral complex of dimension 3.<br>
      <br>
gap> Size(M);<br>
4433<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 255);">The
next command converts M to a homeomorphic regular CW-complex Y with the
same cellular structure as M.<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 204);">gap>
Y:=PermutahedralComplexToRegularCWComplex(M);<br>
Regular CW-complex of dimension 3<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 255);">(The
next
commands
are
not
needed
for the computation of the homomorphism π<sub>1</sub>(δM<sub>K</sub>)
-->
π<sub>1</sub>(M<sub>K</sub>) . They produce a regular CW-complex W
which is
homeomorphic to Y but has fewer cells than Y. The manifold Y has a 4433
3-dimensional cells. The manifold W has just 32 cells of dimension 3.<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 204);">gap>
Y!.nrCells(3);<br>
4433<br>
      <br>
gap> W:=SimplifiedRegularCWComplex(Y);<br>
Regular CW-complex of dimension 3<br>
      <br>
gap> W!.nrCells(3);<br>
32<br>
      <br>
gap>#
                                                                 
)<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 255);">We
now compute the boundary B of Y. This boundary will have two path
components: one will be a surface homeomorphic to a torus, the other
will be homeomorphic to a 2-sphere. <br>
      <br>
By computing the fundamental groups of B based at two different 0-cells
we observe that the 0-cell numbered 35296 lies in the torus. <br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 204);">gap>
B:=BoundaryOfPureComplex(Y);<br>
Regular CW-complex of dimension 2<br>
      <br>
gap> CriticalCellsOfRegularCWComplex(B);<br>
[ [ 2, 1 ], [ 2, 1089 ], [ 1, 3575 ], [ 1, 58055 ], [ 0, 29938 ], [ 0,
35296 ] ]<br>
      <br>
gap> F:=FundamentalGroup(f,29938);<br>
[ <identity ...> ] -> [ <identity ...> ]<br>
      <br>
gap> F:=FundamentalGroup(f,35296);<br>
[ f1, f2 ] -> [ f1^-1*f2^3*f1, f2^-1 ]<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 255);">The
next commands compute a finite presentation for π<sub>1</sub>Y .<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 204);">gap>
pi:=FundamentalGroup(Y);<br>
<fp group of size infinity on the generators [ f1, f2 ]><br>
      <br>
gap> RelatorsOfFpGroup(pi);<br>
[ f1*f2*f1^-1*f2*f1 ]<br>
      </td>
    </tr>
    <tr>
      <td
 style="vertical-align: top; background-color: rgb(255, 255, 255);">In
summary:<br>
      <br>
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 style="text-align: left; width: 40%; margin-left: auto; margin-right: auto;"
 border="0" cellpadding="2" cellspacing="2">
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          <tr>
            <td style="vertical-align: top;">π<sub>1</sub>Y = < x,
y  |  xyx<sup>-1</sup>yx ><br>
            <br>
π<sub>1</sub>B = < u, v  |  uvu<sup>-1</sup>v<sup>-1</sup>
><br>
            <br>
π<sub>1</sub>B ---->  π<sub>1</sub>Y,  u --> x<sup>-1</sup>y<sup>3</sup>x

v
->
y<sup>-1</sup><br>
            </td>
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            <td style="vertical-align: top;"><a
 style="color: rgb(0, 0, 102);" href="aboutKnots.html">Previous
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            <td style="text-align: center; vertical-align: top;"><a
 href="aboutContents.html"><span style="color: rgb(0, 0, 102);">Contents</span></a><br>
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            <td style="text-align: right; vertical-align: top;"><a
 href="aboutCoverinSpaces.html"><span style="color: rgb(0, 0, 102);">Next
page</span><br>
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Messung V0.5
C=95 H=98 G=96

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