Difference between revisions of "Static symmetry"

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{{Ambox|text='''This article needs additional [[Help:Images|images]] for [[hexagonal neighbourhood|hexagonal]] and [[triangular neighbourhood|triangular]] symmetries.'''}}
The Life transition rule, like that of any [[Isotropic_non-totalistic_Life-like_cellular_automaton|isotropic cellular automaton]], is invariant under reflections and rotations. That is, the change in state of a cell remains the same if its [[neighbourhood]] is rotated or reflected. This implies there are '''symmetries''' which if present in a pattern are present in all its successors. Note that the converse is not true: a pattern need not have the full symmetry of one of its successor states.
The Life transition rule, like that of any [[Isotropic_non-totalistic_Life-like_cellular_automaton|isotropic cellular automaton]], is invariant under reflections and rotations. That is, the change in state of a cell remains the same if its [[neighbourhood]] is rotated or reflected. This implies there are '''symmetries''' which if present in a pattern are present in all its successors. Note that the converse is not true: a pattern need not have the full symmetry of one of its successor states.


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|}
|}


To preserve D8_2 symmetry, the following transitions must either all exist simultaneously with all other transitions in the same line or none should:<ref>http://www.conwaylife.com/forums/viewtopic.php?f=11&t=2103&p=28936#p28936</ref>
To preserve D8_2 symmetry, the following transitions must either all exist simultaneously with all other transitions in the same line or none should:<ref name="post28936" />


* B1c/B2c/B4c
* B1c/B2c/B4c
Line 132: Line 133:
If a pattern exhibits symmetry only after its constituent congruent pieces are offset by certain amounts in one or both orthogonal directions, the pattern is said to exhibit skew symmetry.
If a pattern exhibits symmetry only after its constituent congruent pieces are offset by certain amounts in one or both orthogonal directions, the pattern is said to exhibit skew symmetry.


===Gutter symmetries===
===[[Gutter]] symmetries===


Gutter symmetries are distinguished from non-gutter symmetries by the existence of an empty lane of cells &ndash; the "gutter" &ndash; separating the congruent pieces making up overall pattern.
Gutter symmetries are distinguished from non-gutter symmetries by the existence of an empty lane of cells &ndash; the "gutter" &ndash; separating the congruent pieces making up overall pattern.
Line 138: Line 139:
A pattern that exhibits gutter symmetry only after its pieces are skewed in the above sense is said to exhibit skew-gutter symmetry.
A pattern that exhibits gutter symmetry only after its pieces are skewed in the above sense is said to exhibit skew-gutter symmetry.


Gutter and skewgutter symmetries are known to exist for both orthogonal and diagonal lines of symmetry......
Gutter and skewgutter symmetries are known to exist for both orthogonal and diagonal lines of symmetry.........?


{| style="margin-left: auto; margin-right: auto"
{| style="margin-left: auto; margin-right: auto"
|-
|-
| [[File:Symmetry D2 +1g.png|thumb|Orthogonal gutter symmetry]]
| [[File:Symmetry D2_+1g.png|thumb|Orthogonal gutter symmetry<br>D2_+1_gO1S0]]
| [[File:Symmetry D2 +1g s1.png|thumb|Orthogonal skewgutter symmetry]]
| [[File:Symmetry D2_+1g s1.png|thumb|Orthogonal skewgutter symmetry<br>D2_+1_gO1S1]]
| [[File:Symmetry D2 +1g s2.png|thumb|Orthogonal double skewgutter symmetry<ref>http://www.conwaylife.com/forums/viewtopic.php?f=11&t=3120&p=66043#p66043</ref>]]
| [[File:Symmetry D2_+1g s2.png|thumb|Orthogonal double skewgutter symmetry<ref name="post66043" /><br>D2_+1_gO1S2]]
|}
|}


{| style="margin-left: auto; margin-right: auto"
{| style="margin-left: auto; margin-right: auto"
|-
|-
| [[File:Symmetry D2 xg.png|thumb|Diagonal gutter symmetry]]
| [[File:Symmetry D4_+1g.png|thumb|D4_+1 with orthogonal gutter symmetry<br>D4_+1_gO1S0]]
| [[File:Symmetry D2 xg s1.png|thumb|Diagonal skewgutter symmetry]]
| [[File:Symmetry D4_+1gg.png|thumb|D4_+1 with two orthogonal gutters<br>D4_+1_gO1SO_gO1S0]]
| [[File:Symmetry D4_+2g.png|thumb|D4_+2 with orthogonal gutter symmetry<br>D4_+2_gO1S0]]
|}
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Symmetry D4_+2g s1.png|thumb|D4_+2 with orthogonal gutter symmetry, skewed]]
| [[File:Symmetry D4_+2g s2.png|thumb|D4_+2 with orthogonal gutter symmetry, doubly skewed]]
| [[File:Symmetry D4_+1twoskew.png|thumb|D4_+1 with two skew orthogonal gutters]]
|}
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Symmetry D4_+2 twoguttersoneskew.png|thumb|D4_+2 with two orthogonal gutters, one skewed]]
| [[File:Symmetry D4_+2 twoguttersonedoubleskew.png|thumb|D4_+2 with two orthogonal gutters, one doubly skewed]]
| [[File:Symmetry D4_+1twodoubleskew.png|thumb|D4_+1 with two double-skew orthogonal gutters]]
|}
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Symmetry D2_xg.png|thumb|Diagonal gutter symmetry<br>D2_x_gD1S0]]
| [[File:Symmetry D2_xg s1.png|thumb|Diagonal skewgutter symmetry<br>D2_x_gD1S1]]
|}
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Symmetry D4_x1g.png|thumb|D4_x1 with diagonal gutter symmetry<br>D4_x1_gD1S0]]
| [[File:Symmetry D4_x1gg.png|thumb|D4_x1 with two diagonal gutters<br>D4_x1_gD1S0_gD1S0]]
| [[File:Symmetry D4_x4g.png|thumb|D4_x4 with diagonal gutter symmetry<br>D4_x4_gD1S0]]
| [[File:Symmetry D4_x4gg.png|thumb|D4_x4 with two diagonal gutters<br>D4_x4_gD1S0_gD1S0]]
|}
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Symmetry D8_1og.png|thumb|D8_1 with orthogonal gutter symmetry]]
| [[File:Symmetry D8_1dg.png|thumb|D8_1 with diagonal gutter symmetry]]
| [[File:Symmetry D8_1gg.png|thumb|D8_1 with orthogonal and diagonal gutters]]
| [[File:Symmetry D8_4g.png|thumb|D8_4 with diagonal gutter symmetry]]
|}
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Symmetry D8_1s1og.png|thumb|D8_1 with rotationally-symmetric orthogonal skewgutter symmetry]]
| [[File:Symmetry D8_1s1ogdg.png|thumb|and diagonal gutters]]
| [[File:Symmetry D8_1s2og.png|thumb|D8_1 with rotationally-symmetric orthogonal double skewgutter symmetry]]
| [[File:Symmetry D8_1s2ogdg.png|thumb|and diagonal gutters]]
|}
|}


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In order to preserve diagonal skewgutter symmetry, the birth consitions B0, B1c, B1e, B2a, B2k, B3k, B3q and B4q must be absent.
In order to preserve diagonal skewgutter symmetry, the birth consitions B0, B1c, B1e, B2a, B2k, B3k, B3q and B4q must be absent.
Preserving triple or higher orthogonal skewgutter symmetry in a range-1 Moore rule requires that a pattern must not be able to escape its bounding box.
===Compositional/translational symmetry===
For certain rules, any pattern completely made of correctly-aligned arrangements of cells that fit within a 2&times;2 area will always be made up of said 2&times;2 arrangements of cells in all subsequent generations, simulating a [[Margolus]]-neighbourhood rule.<ref name="post54857" /> One famous example of this is [[OCA:2&times;2|2&times;2]].
In the case of 2&times;2's rule, further self-similarity can be noted with certain patterns - anything made of solid 4&times;4 blocks which are correctly aligned will still be made of 4&times;4 blocks in even generations, and so on.
[[apgsearch]] supports the full block version of these symmetries through the inflation operator.
===Oscillator symmetries===
[[Oscillators]] have a wider range of symmetries than still lifes. This is because an oscillator can appear in two or four congruent states, not necessarily the same. There are 43 possible symmetries of oscillators, 27 of which do not appear in still lifes (i.e. period/mod = 2 or 4). The symmetry class is the symmetry class of the oscillator in a single generation followed by the symmetry class of the union of the generation and its congruent successors.<ref>{{CiteHickersonOscillators|accessdate=May 2, 2019}}</ref><!--
====Flippers====
====180 degree rotators====
====90 degree rotators====-->
===Spaceship symmetries===
Spaceships have a limited range of symmetries because no spaceship can have rotational symmetry. However, spaceships can have glide symmetry, which is not applicable for finite patterns that do not move.


==Hexagonal-grid and triangular-grid symmetries==
==Hexagonal-grid and triangular-grid symmetries==


[[hexagonal neighbourhood|Hexagonal]] and [[triangular neighbourhood|triangular]] grids do not have the same symmetries as square grids. C2, D2, and D4 symmetries are still compatible, but C4 symmetries become meaningless because the cells no longer have a side count that is divisible by 4. Other symmetries are exclusive to these alternative grids, such as C3_1, C3_3, D6_1, and D6_3. C6 and D12 symmetries are also possible in a hexagon-tiled universe.
[[hexagonal neighbourhood|Hexagonal]] and [[triangular neighbourhood|triangular]] grids have the same set of admissible symmetries as each other (by [http://mathworld.wolfram.com/DualTessellation.html planar duality]), but these are not the same symmetries as square grids. Due to how hexagonal and triangular grids are handled by programs such as [[Golly]] and [[LifeViewer]], they will also appear markedly different in these respects. C2, D2, and D4 symmetries are still compatible, but C4 symmetries become meaningless because the cells no longer have a side count that is perfectly divisible by 4. Other symmetries are exclusive to these alternative grids, as indicated below:


[[apgsearch]] does not currently support all higher symmetries for hexagonal rules, but all will be added in a future version.<ref>{{LinkForumThread|format=ref|title=Re: Non-totalistic hex rules|p=66090|author=Adam P. Goucher}}</ref>
* C1
* C2_1
* C2_4
* C3_1
* C3_3 (unsupported by apgsearch)
* C6
* D2_xo
* D2_x
* D4_x1
* D4_x4
* D6_1
* D6_1o
* D6_3 (unsupported by apgsearch)
* D12
 
[[apgsearch]] currently supports most higher symmetries for hexagonal rules; the rest (C3_3 and D6_3) will be added in a future version.<ref name="post66638" />
 
Hexagonal rules can also support gutter symmetry,<ref name="post66215" /> however, like with square grid gutters, apgsearch does not currently support searching with these.
 
===Rotational symmetries===
Rotational symmetries include the following:
 
====C1====
'''C1''': Symmetric under 360° rotation. This is essentially no symmetry at all.
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Hexagonal symmetry C1.png|frame|C1 symmetry]]
|}
 
====C2====
'''C2''': Symmetric under 180° rotation. There are two possibilities:
 
* '''C2_1''': Rotation around the center of a cell.
* '''C2_4''': Rotation around a corner of a cell.
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Hexagonal symmetry C2_1.png|frame|C2_1 symmetry]]
| [[File:Hexagonal symmetry C2_4.png|frame|C2_4 symmetry]]
|}
 
====C3====
'''C3''': Symmetric under 120° rotation. There are two possibilities:
 
* '''C3_1''': Rotation around the center of a cell.
* '''C3_3''': Rotation around a corner of a cell. (unsupported by apgsearch)
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Hexagonal symmetry C3_1.png|frame|C3_1 symmetry]]
| [[File:Hexagonal symmetry C3_3.png|frame|C3_3 symmetry]]
|}
 
====C6====
'''C6''': Symmetric under 60° rotation.
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Hexagonal symmetry C6.png|frame|C6 symmetry]]
|}
 
===Reflectional symmetries===
Reflectional symmetries include the following:
 
====D2====
'''D2''': There is line symmetry. There are two possibilities:
 
* '''D2_x''': Through the vertices of a cell.
* '''D2_xo''': Through the edges of a cell.
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Hexagonal symmetry D2_x.png|frame|D2_x symmetry]]
| [[File:Hexagonal symmetry D2_xo.png|frame|D2_xo symmetry]]
|}
 
====D4====
'''D4''': Symmetric under both reflection and 180° rotation. The reflection symmetry will be with respect to two lines. There are two possibilities:
 
* '''D4_x1''': Rotation around the center of a cell.
* '''D4_x4''': Rotation around the edges of a cell.
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Hexagonal symmetry D4_x1.png|frame|D4_x1 symmetry]]
| [[File:Hexagonal symmetry D4_x4.png|frame|D4_x4 symmetry]]
|}
 
====D6====
'''D6''': Symmetric under both reflection and 120° rotation. The reflection symmetry will be with respect to three lines. There are three possibilities:
 
* '''D6_1''': Rotation around the center of a cell with lines going through the edges of cells.
* '''D6_1o''': Rotation around the center of a cell with lines going through the centers of cells.
* '''D6_3''': Rotation around the corner of a cell. (unsupported by apgsearch)
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Hexagonal symmetry D6_1.png|frame|D6_1 symmetry]]
| [[File:Hexagonal symmetry D6_1o.png|frame|D6_1o symmetry]]
| [[File:Hexagonal symmetry D6_3.png|frame|D6_3 symmetry]]
|}
 
====D12====
'''D12''': Symmetric under both reflection and 60° rotation. The reflection symmetry will be with respect to six lines.
 
{| style="margin-left: auto; margin-right: auto"
|-
| [[File:Hexagonal symmetry D12.png|frame|D12 symmetry]]
|}


==References==
==References==
<references />
<references>
<ref name="post28936">{{LinkForumThread
|format = ref
|title  = Truly Bilateral Life-Like rules
|p      = 28936
|author = BlinkerSpawn
|date  = March 19, 2016
}}</ref>
<ref name="post66043">{{LinkForumThread
|format = ref
|title  = Re: Rules with interesting dynamics
|p      = 66043
|author = muzik
|date  = November 30, 2018
}}</ref>
<ref name="post66215">{{LinkForumThread
|format = ref
|title  = Re: Non-totalistic hex rules
|p      = 66215
|author = muzik
|date  = December 5, 2018
}}</ref>
<ref name="post66638">{{LinkForumThread
|format = ref
|title  = Re: apgsearch v4.0
|p      = 66638
|author = Adam P. Goucher
|date  = December 20, 2018
}}</ref>
<ref name="post54857">{{LinkForumThread
|format = ref
|title  = Re: Rules with interesting dynamics
|p      = 54857
|author = Aidan F. Pierce
|date  = January 8, 2018
}}</ref>
</references>


==External links==
==External links==
{{LinkLexicon|lex_s.htm#symmetric|name=Symmetric}}
{{LinkForumThread|f=7|t=1898|title=Help with symmetries}}
{{LinkForumThread|f=7|t=1898|title=Help with symmetries}}


[[Category:Everything else]]
[[Category:Everything else]]
__NOTOC__

Revision as of 20:48, 15 January 2020

Ambox notice.png This article needs additional images for hexagonal and triangular symmetries.

The Life transition rule, like that of any isotropic cellular automaton, is invariant under reflections and rotations. That is, the change in state of a cell remains the same if its neighbourhood is rotated or reflected. This implies there are symmetries which if present in a pattern are present in all its successors. Note that the converse is not true: a pattern need not have the full symmetry of one of its successor states.

Square-grid symmetries

Overview of symmetries (excluding D8_2).

Rotational symmetries

Rotational symmetries include the following (note that "C" refers to the cyclic groups):

C1

C1: Symmetric under 360° rotation. This is essentially no symmetry at all.

C1 symmetry

C2

C2: Symmetric under 180° rotation. There are three possibilities:

  • C2_1: Rotation around the center of a cell. The bounding rectangle of a C2_1 pattern is odd by odd.
  • C2_2: Rotation around the midpoint of a side of a cell. The bounding rectangle is even by odd.
  • C2_4: Rotation around a corner of a cell. The bounding rectangle is even by even.
C2_1 symmetry
C2_2 symmetry
C2_4 symmetry

C4

C4: Symmetric under 90° rotation. There are two possibilities:

  • C4_1: Rotation around the center of a cell. The bounding rectangle is odd by odd.
  • C4_4: Rotation around a corner of a cell. The bounding rectangle is even by even.
C4_1 symmetry
C4_4 symmetry

Reflectional symmetries

Reflectional symmetries include the following (note that "D" refers to the dihedral groups):

D2

D2: Symmetric under reflection through a line. There are two possibilities:

  • D2_+ The line is orthogonal. There are two sub-possibilities:
    • D2_+1 The line bisects a row of cells. The bounding rectangle is odd by any.
    • D2_+2 The line lies between two rows of cells. The bounding rectangle is even by any.
D2_+1 symmetry
D2_+2 symmetry
  • D2_x The line is diagonal.
D2_x symmetry

D4

D4: Symmetric under both reflection and 180° rotation. The reflection symmetry will be with respect to two lines. There are two possibilities:

  • D4_+: The lines are orthogonal. There are three sub-possibilities:
    • D4_+1: Rotation around the center of a cell. The bounding rectangle is odd by odd.
    • D4_+2: Rotation around the midpoint of a side of a cell. The bounding rectangle is even by odd.
    • D4_+4: Rotation around a corner of a cell. The bounding rectangle is even by even.
D4_+1 symmetry
D4_+2 symmetry
D4_+4 symmetry
  • D4_x The lines are diagonal. There are two sub-possibilities:
    • D4_x1: Rotation around the center of a cell. The bounding rectangle is odd by odd.
    • D4_x4: Rotation around a corner of a cell. The bounding rectangle is even by even.
D4_x1 symmetry
D4_x4 symmetry

D8

D8: Symmetric under both reflection and 90° rotation. The reflection symmetry will be with respect to horizontal, vertical, and diagonal lines. There are two possibilities:

  • D8_1: Rotation around the center of a cell. The bounding rectangle is odd by odd.
  • D8_2: Rotation around a edge of a cell. The bounding rectangle is even by odd. This symmetry is not preserved by Life (reverting to D4_+2), but is with most bilaterally symmetric rules.
  • D8_4: Rotation around a corner of a cell. The bounding rectangle is even by even.
D8_1 symmetry
D8_2 symmetry
D8_4 symmetry

To preserve D8_2 symmetry, the following transitions must either all exist simultaneously with all other transitions in the same line or none should:[1]

  • B1c/B2c/B4c
  • B1e/B2a/B2i/B4i
  • B3e/B3j
  • B3i/B6i
  • B3q/B3y
  • B4t/B5r
  • B4e/B5y/B4w
  • B4a/B5i
  • B4n/B5e
  • B5a/B7e/B8
  • B6c/B6k
  • S0/S1e/S3a
  • S2c/S2k
  • S2i/S5i
  • S3e/S4r
  • S3i/S4a/S4t/S6a/S6i/S7e
  • S3r/S4i
  • S3y/S4c/S4q
  • S5e/S5j
  • S5q/S5y
  • S6c/S7c

Skew symmetries

If a pattern exhibits symmetry only after its constituent congruent pieces are offset by certain amounts in one or both orthogonal directions, the pattern is said to exhibit skew symmetry.

Gutter symmetries

Gutter symmetries are distinguished from non-gutter symmetries by the existence of an empty lane of cells – the "gutter" – separating the congruent pieces making up overall pattern.

A pattern that exhibits gutter symmetry only after its pieces are skewed in the above sense is said to exhibit skew-gutter symmetry.

Gutter and skewgutter symmetries are known to exist for both orthogonal and diagonal lines of symmetry.........?

Orthogonal gutter symmetry
D2_+1_gO1S0
Orthogonal skewgutter symmetry
D2_+1_gO1S1
Orthogonal double skewgutter symmetry[2]
D2_+1_gO1S2
D4_+1 with orthogonal gutter symmetry
D4_+1_gO1S0
D4_+1 with two orthogonal gutters
D4_+1_gO1SO_gO1S0
D4_+2 with orthogonal gutter symmetry
D4_+2_gO1S0
D4_+2 with orthogonal gutter symmetry, skewed
D4_+2 with orthogonal gutter symmetry, doubly skewed
D4_+1 with two skew orthogonal gutters
D4_+2 with two orthogonal gutters, one skewed
D4_+2 with two orthogonal gutters, one doubly skewed
D4_+1 with two double-skew orthogonal gutters
Diagonal gutter symmetry
D2_x_gD1S0
Diagonal skewgutter symmetry
D2_x_gD1S1
D4_x1 with diagonal gutter symmetry
D4_x1_gD1S0
D4_x1 with two diagonal gutters
D4_x1_gD1S0_gD1S0
D4_x4 with diagonal gutter symmetry
D4_x4_gD1S0
D4_x4 with two diagonal gutters
D4_x4_gD1S0_gD1S0
D8_1 with orthogonal gutter symmetry
D8_1 with diagonal gutter symmetry
D8_1 with orthogonal and diagonal gutters
D8_4 with diagonal gutter symmetry
D8_1 with rotationally-symmetric orthogonal skewgutter symmetry
and diagonal gutters
D8_1 with rotationally-symmetric orthogonal double skewgutter symmetry
and diagonal gutters

In order to preserve orthogonal gutter symmetry, the birth conditions B0, B2c, B2i, B4i, B4c and B6i must be absent.

In order to preserve orthogonal skewgutter symmetry, the birth conditions B0, B1c, B2k, B2n, B3n, B3y, B4y, B4z, B5r and B6i must be absent.

In order to preserve orthogonal double skewgutter symmetry, the birth conditions B0, B1c, B1e, B2a, B2i, B2k, B2n, B3c, B3q, B3r, B4c, B4n, B4y, B4z, B5e, B5r and B6i must be absent.

In order to preserve diagonal gutter symmetry, the birth conditions B0, B2n, B2e, B4e, B4w and B6n must be absent.

In order to preserve diagonal skewgutter symmetry, the birth consitions B0, B1c, B1e, B2a, B2k, B3k, B3q and B4q must be absent.

Preserving triple or higher orthogonal skewgutter symmetry in a range-1 Moore rule requires that a pattern must not be able to escape its bounding box.

Compositional/translational symmetry

For certain rules, any pattern completely made of correctly-aligned arrangements of cells that fit within a 2×2 area will always be made up of said 2×2 arrangements of cells in all subsequent generations, simulating a Margolus-neighbourhood rule.[3] One famous example of this is 2×2.

In the case of 2×2's rule, further self-similarity can be noted with certain patterns - anything made of solid 4×4 blocks which are correctly aligned will still be made of 4×4 blocks in even generations, and so on.

apgsearch supports the full block version of these symmetries through the inflation operator.

Oscillator symmetries

Oscillators have a wider range of symmetries than still lifes. This is because an oscillator can appear in two or four congruent states, not necessarily the same. There are 43 possible symmetries of oscillators, 27 of which do not appear in still lifes (i.e. period/mod = 2 or 4). The symmetry class is the symmetry class of the oscillator in a single generation followed by the symmetry class of the union of the generation and its congruent successors.[4]

Spaceship symmetries

Spaceships have a limited range of symmetries because no spaceship can have rotational symmetry. However, spaceships can have glide symmetry, which is not applicable for finite patterns that do not move.

Hexagonal-grid and triangular-grid symmetries

Hexagonal and triangular grids have the same set of admissible symmetries as each other (by planar duality), but these are not the same symmetries as square grids. Due to how hexagonal and triangular grids are handled by programs such as Golly and LifeViewer, they will also appear markedly different in these respects. C2, D2, and D4 symmetries are still compatible, but C4 symmetries become meaningless because the cells no longer have a side count that is perfectly divisible by 4. Other symmetries are exclusive to these alternative grids, as indicated below:

  • C1
  • C2_1
  • C2_4
  • C3_1
  • C3_3 (unsupported by apgsearch)
  • C6
  • D2_xo
  • D2_x
  • D4_x1
  • D4_x4
  • D6_1
  • D6_1o
  • D6_3 (unsupported by apgsearch)
  • D12

apgsearch currently supports most higher symmetries for hexagonal rules; the rest (C3_3 and D6_3) will be added in a future version.[5]

Hexagonal rules can also support gutter symmetry,[6] however, like with square grid gutters, apgsearch does not currently support searching with these.

Rotational symmetries

Rotational symmetries include the following:

C1

C1: Symmetric under 360° rotation. This is essentially no symmetry at all.

C2

C2: Symmetric under 180° rotation. There are two possibilities:

  • C2_1: Rotation around the center of a cell.
  • C2_4: Rotation around a corner of a cell.

C3

C3: Symmetric under 120° rotation. There are two possibilities:

  • C3_1: Rotation around the center of a cell.
  • C3_3: Rotation around a corner of a cell. (unsupported by apgsearch)

C6

C6: Symmetric under 60° rotation.

Reflectional symmetries

Reflectional symmetries include the following:

D2

D2: There is line symmetry. There are two possibilities:

  • D2_x: Through the vertices of a cell.
  • D2_xo: Through the edges of a cell.

D4

D4: Symmetric under both reflection and 180° rotation. The reflection symmetry will be with respect to two lines. There are two possibilities:

  • D4_x1: Rotation around the center of a cell.
  • D4_x4: Rotation around the edges of a cell.

D6

D6: Symmetric under both reflection and 120° rotation. The reflection symmetry will be with respect to three lines. There are three possibilities:

  • D6_1: Rotation around the center of a cell with lines going through the edges of cells.
  • D6_1o: Rotation around the center of a cell with lines going through the centers of cells.
  • D6_3: Rotation around the corner of a cell. (unsupported by apgsearch)

D12

D12: Symmetric under both reflection and 60° rotation. The reflection symmetry will be with respect to six lines.

References

  1. BlinkerSpawn (March 19, 2016). Truly Bilateral Life-Like rules (discussion thread) at the ConwayLife.com forums
  2. muzik (November 30, 2018). Re: Rules with interesting dynamics (discussion thread) at the ConwayLife.com forums
  3. Aidan F. Pierce (January 8, 2018). Re: Rules with interesting dynamics (discussion thread) at the ConwayLife.com forums
  4. Dean Hickerson's oscillator stamp collection. Retrieved on May 2, 2019.
  5. Adam P. Goucher (December 20, 2018). Re: apgsearch v4.0 (discussion thread) at the ConwayLife.com forums
  6. muzik (December 5, 2018). Re: Non-totalistic hex rules (discussion thread) at the ConwayLife.com forums

External links