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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}](img37.gif) |
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}](img38.gif) |
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}](img39.gif) |
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}](img40.gif) |
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}](img41.gif) |
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}](img42.gif) |
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}](img43.gif) |
Next: participating gliders
Up: T8
Previous: cross references
  Contents
Jose Manuel Gomez Soto
2002-05-15