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periodic lattice component

Figure: T8's can still be stacked diagonally to produce a light velocity lattice. They require T1's to fill the interstices.
\begin{figure}\centering\begin{picture}(160,100) \put(0,0){\epsfxsize =160pt \epsffile{light8.eps}} \end{picture}\end{figure}

Figure: T8's can be strung out along horizontal rows, either rising or falling.
\begin{figure}\centering\begin{picture}(260,150) \put(0,0){\epsfxsize =260pt \ep... ...} \put(0,80){\epsfxsize =260pt \epsffile{t8r9in1.eps}} \end{picture}\end{figure}

Figure: A horizontal row of T8's can also rise slightly more rapidly [left 9 in 2] than in the figure above.
\begin{figure}\centering\begin{picture}(260,70) \put(0,0){\epsfxsize =260pt \epsffile{t8l9in2.eps}} \end{picture}\end{figure}

Figure: Falling rows of T8's.
\begin{figure}\centering\begin{picture}(260,80) \put(0,0){\epsfxsize =260pt \epsffile{t8r7in3.eps}} \end{picture}\end{figure}

Figure: Falling rows, nearly diagonals, can arise even though the T8's are not contiguous and include other large triangles.
\begin{figure}\centering\begin{picture}(290,180) \put(15,0){\epsfxsize =260pt \e... ...} \put(0,90){\epsfxsize =290pt \epsffile{t8r9in6.eps}} \end{picture}\end{figure}

Figure: Two different families of diagonal stripes featuring T8's. In each case the stripes are separated in their own way.
\begin{figure}\centering\begin{picture}(290,160) \put(15,0){\epsfxsize =260pt \e... ...} \put(0,90){\epsfxsize =290pt \epsffile{t8l9in6.eps}} \end{picture}\end{figure}

Figure: T8's can form nearly vertical stripes, separated by optional vertical stripes of T2's (which, however, cannot be juxtaposed), and possiblt terminating a T5 lattice on its right.
\begin{figure}\centering\begin{picture}(260,80) \put(0,0){\epsfxsize =260pt \epsffile{t8l4in9.eps}} \end{picture}\end{figure}

next up previous contents
Next: participating gliders Up: T8 Previous: cross references   Contents
Jose Manuel Gomez Soto 2002-05-15