Table file:

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`n_states:3`

neighborhood:Moore

symmetries:permute

var a={1,2}

var b={1,2}

var c={1,2}

var d={1,2}

var e={1,2}

var f={1,2}

var s={0,1,2}

var t={0,1,2}

var u={0,1,2}

var v={0,1,2}

var w={0,1,2}

var x={0,1,2}

var y={0,1,2}

var z={0,1,2}

1,s,t,a,b,c,d,e,f,0

1,0,0,0,0,a,b,c,d,0

1,0,0,0,0,0,0,c,d,0

1,0,0,0,0,0,0,0,0,0

2,s,t,a,b,c,d,e,f,0

2,0,0,0,0,s,t,u,v,0

0,1,1,1,0,0,0,0,0,2

0,2,2,0,0,0,0,0,0,1

1,s,t,u,v,w,x,y,z,2

2,s,t,u,v,w,x,y,z,1

Random patterns tend to become dominated by simple p4 oscillators. There is an extremely common c/2 p4 spaceship:

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`#CXRLE Pos=-15,-8`

x = 6, y = 7, rule = jelly

2A2.2A2$2.2A3$A4.A$A.2A.A!

And this rarer variant:

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`#CXRLE Pos=-21,-19`

x = 5, y = 4, rule = jelly

.A.A$A3.A2$A.A!

Of particular interest is this c/2 p22 ship which shows up rarely. It can form a variety of puffers:

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`#CXRLE Pos=-15,-8`

x = 6, y = 7, rule = jelly

2A2.2A2$2.2A3$A4.A$A.2A.A!

Another interesting feature is this replicator:

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`x = 1, y = 8, rule = jelly`

A$A5$A$A!

Which duplicates itself 4 cells in 14 gens. It can be stabilised into a p28 oscillator:

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`#CXRLE Pos=-30,-11`

x = 20, y = 10, rule = jelly

.A17.A$A11.A5.A$12.A5$12.A$A11.A5.A$.A17.A!

Two copies of it are used in this, a 2c/7 spaceship:

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`x = 27, y = 72, rule = Jelly`

4.2B4.2B7.2B4.2B7$17.3B$3.B8.B5.2B$3.B8.B4.2B$3.B.B.2B.B.B4.B3.B3.2B$

3.B8.B3.B4.B$3.B8.B4.B4.B8$4.2B4.2B24$4.B$3.B3$11.B3.B$12.B.B13$4.B.

3B$2.B3.4B$.B6.B.B$.2B.2B$B2.B2$10.B$10.B.B$8.B.2B$9.B!

So yeah.