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Incidence structure
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===Incidence matrix=== {{main|Incidence matrix}} The '''incidence matrix''' of a (finite) incidence structure is a [[(0,1) matrix]] that has its rows indexed by the points {{mvar|{p<sub>i</sub>} }} and columns indexed by the lines {{math|{''l<sub>j</sub>''} }} where the {{mvar|ij}}-th entry is a 1 if {{math|''p<sub>i</sub>'' I ''l<sub>j</sub>''}} and 0 otherwise.{{efn|The other convention of indexing the rows by lines and the columns by points is also widely used.}} An incidence matrix is not uniquely determined since it depends upon the arbitrary ordering of the points and the lines.<ref name=Beth17>{{harvnb|Beth|Jungnickel|Lenz|1986|page=17}}</ref> The non-uniform incidence structure pictured above (example number 2) is given by: <math display=block>\begin{align} P &= \{ A, B, C, D, E, P \} \\[2pt] L &= \left\{ \begin{array}{ll} l = \{C, P, E \}, & m = \{ P \}, \\ n = \{ P, D \}, & o = \{ P, A \}, \\ p = \{ A, B \}, & q = \{ P, B \} \end{array} \right\} \end{align}</math> An incidence matrix for this structure is: <math display="block"> \begin{pmatrix} 0 & 0 & 0 & 1 & 1 & 0 \\ 0 & 0 & 0 & 0 & 1 & 1 \\ 1 & 0 & 0 & 0 & 0 & 0 \\ 0 & 0 & 1 & 0 & 0 & 0 \\ 1 & 0 & 0 & 0 & 0 & 0 \\ 1 & 1 & 1 & 1 & 0 & 1 \end{pmatrix} </math> which corresponds to the incidence table: {| class="wikitable" style="text-align:center; width=200px; height=200px;" |- ! {{math|I}} !! {{mvar|l}} !! {{mvar|m}} !! {{mvar|n}} !! {{mvar|o}} !! {{mvar|p}} !! {{mvar|q}} |- ! {{mvar|A}} | 0 || 0 || 0 || 1 || 1 || 0 |- ! {{mvar|B}} | 0 || 0 || 0 || 0 || 1 || 1 |- ! {{mvar|C}} | 1 || 0 || 0 || 0 || 0 || 0 |- ! {{mvar|D}} | 0 || 0 || 1 || 0 || 0 || 0 |- ! {{mvar|E}} | 1 || 0 || 0 || 0 || 0 || 0 |- ! {{mvar|P}} | 1 || 1 || 1 || 1 || 0 || 1 |} If an incidence structure {{mvar|C}} has an incidence matrix {{mvar|M}}, then the dual structure {{math|''C''<sup>β</sup>}} has the [[transpose matrix]] {{mvar|M}}<sup>T</sup> as its incidence matrix (and is defined by that matrix). An incidence structure is self-dual if there exists an ordering of the points and lines so that the incidence matrix constructed with that ordering is a [[symmetric matrix]]. With the labels as given in example number 1 above and with points ordered {{math|''A'', ''B'', ''C'', ''D'', ''G'', ''F'', ''E''}} and lines ordered {{math|''l'', ''p'', ''n'', ''s'', ''r'', ''m'', ''q''}}, the Fano plane has the incidence matrix: <math display="block"> \begin{pmatrix} 1 & 1 & 1 & 0 & 0 & 0 & 0\\ 1 & 0 & 0 & 1 & 1 & 0 & 0 \\ 1 & 0 & 0 & 0 & 0 & 1 & 1 \\ 0 & 1 & 0 & 1 & 0 & 1 & 0 \\ 0 & 1 & 0 & 0 & 1 & 0 & 1 \\ 0 & 0 & 1 & 1 & 0 & 0 & 1 \\ 0 & 0 & 1 & 0 & 1 & 1 & 0 \end{pmatrix} . </math> Since this is a symmetric matrix, the Fano plane is a self-dual incidence structure.
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