periodic lattice component

**Figure:** Although the T6's will not fit together in a lattice of which they are the only component, they go well with T1's, in two enantiomorphic forms.
$\begin{figure}\centering\begin{picture}(260,100) \put(0,10){\epsfxsize =120pt \e... ...s}} \put(160,0){\epsfxsize =100pt \epsffile{t06b.eps}} \end{picture}\end{figure}$

**Figure:** However, the symmetric form in which T6's repeat along the diagonal to make a light velocity lattice, is impossible.
$\begin{figure}\centering\begin{picture}(140,40) \put(0,-10){\epsfxsize =140pt \epsffile{t06c.eps}} \end{picture}\end{figure}$

Table: The columnar form of stacked T6's is C gliders, which show up in superluminal form in various parts of the map. Diagonal stacking is also possible, with a high position marked hi and a low position marked lo. In the subluminal region some composites are possible, marked HI or LO. Many other, less simple, combinations are possible.

	10	9	8	7	6	5	4	3	2	1	0	1	2	3	4	5	6	7	8	9	10
1	.	.	.	.	.	.	.	.	.	*	.	*	.	.	.	.	.	.	.	.	.
2	.	.	.	.	.	.	.	.	*	.	.	.	*	.	.	.	.	.	.	.	.
3	.	C3	.	.	.	.	.	*	.	.	.	.	.	*	.	.	hi	.	.	C3	lo
4	.	.	.	hi	.	.	*	.	.	.	.	.	.	.	*	.	.	.	.	C3	.
5	.	C2	.	.	.	*	.	.	.	.	.	.	.	lo	.	*	.	.	.	.	.
6	.	.	.	.	*	.	.	.	.	.	.	.	.	.	.	.	*	.	.	.	hi
7	.	C1	.	.	.	.	LO	.	HI	.	.	.	.	.	.	.	.	*	.	C1	.
8	.	.	*	.	.	.	.	.	.	.	.	.	.	.	.	.	.	.	*	.	.
9	.	*	.	.	.	.	.	.	.	.	.	.	.	.	.	.	.	.	.	C2	.
10	*	.	.	.	.	.	.	.	.	.	.	.	.	hi	.	.	lo	.	.	.	*

**Figure:** T6 is the largest triangle in the C gliders. The three C's are distinguished by the alignment of T6's and T1's wherever two columns join. The C gliders pack readily into lattices. An enormous variety eventually results from varying the staggering from column to column.
$\begin{figure}\centering\begin{picture}(400,320) \put(0,0){\epsfxsize =400pt \epsffile{c1c2c3.eps}} \end{picture}\end{figure}$

**Figure:** Columns which somewhat resemble the C gliders result when the T6's are separated by padding of the same width.
$\begin{figure}\centering\begin{picture}(400,120) \put(0,0){\epsfxsize =400pt \epsffile{t6cy84.eps}} \end{picture}\end{figure}$

**Figure:** The same unit cell from Fig. gives another lattice when its alignment is changed, this time with a steeper diagonal slant.
$\begin{figure}\centering\begin{picture}(380,160) \put(0,0){\epsfxsize =380pt \epsffile{t6cy14.eps}} \end{picture}\end{figure}$

**Figure:** Three more variations on a slanting theme.
$\begin{figure}\centering\begin{picture}(380,320) \put(100,260){\epsfxsize =200pt... ... \put(0,140){\epsfxsize =380pt \epsffile{t6cy101.eps}} \end{picture}\end{figure}$

**Figure:** Another three variations on a downward slanting theme.
$\begin{figure}\centering\begin{picture}(340,390) \put(0,290){\epsfxsize =340pt \... ... \put(0,140){\epsfxsize =340pt \epsffile{t6cy190.eps}} \end{picture}\end{figure}$

**Figure:** A lattice in which a T6 and a T7 share a unit cell.
$\begin{figure}\centering\begin{picture}(380,100) \put(0,0){\epsfxsize =380pt \epsffile{t6cy25.eps}} \end{picture}\end{figure}$

**Figure:** A much more complex T6 lattice, of cycle 372, corresponding to 10 right every 9 generations. Note the family resemblance to the middle image in Fig where only two T4's mesh with T6's.
$\begin{figure}\centering\begin{picture}(400,140) \put(0,0){\epsfxsize =400pt \epsffile{t6cy372.eps}} \end{picture}\end{figure}$