Conway polyhedron notation

In geometry and topology, Conway polyhedron notation, invented by John Horton Conway and promoted by George W. Hart, is used to describe polyhedra based on a seed polyhedron modified by various prefix operations.^[1][2]

Conway and Hart extended the idea of using operators, like

. Some basic operations can be made as composites of others: for instance, ambo applied twice is the expand operation (aa = e), while a truncation after ambo produces bevel (ta = b).

Polyhedra can be studied topologically, in terms of how their vertices, edges, and faces connect together, or geometrically, in terms of the placement of those elements in space. Different implementations of these operators may create polyhedra that are geometrically different but topologically equivalent. These topologically equivalent polyhedra can be thought of as one of many

canonical form

to avoid ambiguity.

Operators

In Conway's notation, operations on polyhedra are applied like functions, from right to left. For example, a cuboctahedron is an ambo cube,^[6] i.e. ${\displaystyle a(C)=aC}$, and a truncated cuboctahedron is ${\displaystyle t(a(C))=t(aC)=taC}$. Repeated application of an operator can be denoted with an exponent: j² = o. In general, Conway operators are not

.

Individual operators can be visualized in terms of

LSPs should be understood as local operations that preserve symmetry, not operations that preserve local symmetry. Again, these are symmetries in a topological sense, not a geometric sense: the exact angles and edge lengths may differ.

Fundamental domains of faces with ${\displaystyle n}$ sides

3 (Triangle)	4 (Square)	5 (Pentagon)	6 (Hexagon)
The fundamental domains for polyhedron groups. The groups are ${\displaystyle D_{3},D_{4},D_{5},D_{6}}$ for achiral polyhedra, and ${\displaystyle C_{3},C_{4},C_{5},C_{6}}$ for chiral polyhedra.

Hart introduced the reflection operator r, that gives the mirror image of the polyhedron.[6] This is not strictly a LOPSP, since it does not preserve orientation: it reverses it, by exchanging white and red chambers. r has no effect on achiral polyhedra aside from orientation, and rr = S returns the original polyhedron. An overline can be used to indicate the other chiral form of an operator: s = rsr.

An operation is irreducible if it cannot be expressed as a composition of operators aside from d and r. The majority of Conway's original operators are irreducible: the exceptions are e, b, o, and m.

Matrix representation

x	${\displaystyle {\begin{bmatrix}a&b&c\\0&d&0\\a'&b'&c'\end{bmatrix}}=\mathbf {M} _{x}}$
xd	${\displaystyle {\begin{bmatrix}c&b&a\\0&d&0\\c'&b'&a'\end{bmatrix}}=\mathbf {M} _{x}\mathbf {M} _{d}}$
dx	${\displaystyle {\begin{bmatrix}a'&b'&c'\\0&d&0\\a&b&c\end{bmatrix}}=\mathbf {M} _{d}\mathbf {M} _{x}}$
dxd	${\displaystyle {\begin{bmatrix}c'&b'&a'\\0&d&0\\c&b&a\end{bmatrix}}=\mathbf {M} _{d}\mathbf {M} _{x}\mathbf {M} _{d}}$

The relationship between the number of vertices, edges, and faces of the seed and the polyhedron created by the operations listed in this article can be expressed as a matrix ${\displaystyle \mathbf {M} _{x}}$. When x is the operator, ${\displaystyle v,e,f}$ are the vertices, edges, and faces of the seed (respectively), and ${\displaystyle v',e',f'}$ are the vertices, edges, and faces of the result, then

${\displaystyle \mathbf {M} _{x}{\begin{bmatrix}v\\e\\f\end{bmatrix}}={\begin{bmatrix}v'\\e'\\f'\end{bmatrix}}}$.

The matrix for the composition of two operators is just the product of the matrixes for the two operators. Distinct operators may have the same matrix, for example, p and l. The edge count of the result is an integer multiple d of that of the seed: this is called the inflation rate, or the edge factor.^[7]

The simplest operators, the

d, have simple matrix forms:

${\displaystyle \mathbf {M} _{S}={\begin{bmatrix}1&0&0\\0&1&0\\0&0&1\end{bmatrix}}=\mathbf {I} _{3}}$, ${\displaystyle \mathbf {M} _{d}={\begin{bmatrix}0&0&1\\0&1&0\\1&0&0\end{bmatrix}}}$

Two dual operators cancel out; dd = S, and the square of ${\displaystyle \mathbf {M} _{d}}$ is the identity matrix. When applied to other operators, the dual operator corresponds to horizontal and vertical reflections of the matrix. Operators can be grouped into groups of four (or fewer if some forms are the same) by identifying the operators x, xd (operator of dual), dx (dual of operator), and dxd (conjugate of operator). In this article, only the matrix for x is given, since the others are simple reflections.

Number of operators

The number of LSPs for each inflation rate is ${\displaystyle 2,2,4,6,6,20,28,58,82,\cdots }$ starting with inflation rate 1. However, not all LSPs necessarily produce a polyhedron whose edges and vertices form a 3-connected graph, and as a consequence of Steinitz's theorem do not necessarily produce a convex polyhedron from a convex seed. The number of 3-connected LSPs for each inflation rate is ${\displaystyle 2,2,4,6,4,20,20,54,64,\cdots }$.^[8]

Original operations

Strictly, seed (S), needle (n), and zip (z) were not included by Conway, but they are related to original Conway operations by duality so are included here.

From here on, operations are visualized on cube seeds, drawn on the surface of that cube. Blue faces cross edges of the seed, and pink faces lie over vertices of the seed. There is some flexibility in the exact placement of vertices, especially with chiral operators.

Original Conway operators

Edge factor	Matrix ${\displaystyle \mathbf {M} _{x}}$	x	xd	dx	dxd	Notes
1	${\displaystyle {\begin{bmatrix}1&0&0\\0&1&0\\0&0&1\end{bmatrix}}}$	Seed: S	Dual: d		Seed: dd = S	Dual replaces each face with a vertex, and each vertex with a face.
2	${\displaystyle {\begin{bmatrix}1&0&1\\0&2&0\\0&1&0\end{bmatrix}}}$	Join: j		Ambo: a		Join creates quadrilateral faces. Ambo creates degree-4 vertices, and is also called rectification, or the medial graph in graph theory.[10]
3	${\displaystyle {\begin{bmatrix}1&0&1\\0&3&0\\0&2&0\end{bmatrix}}}$	Kis: k	Needle: n	Zip: z	Truncate: t	Kis raises a pyramid on each face, and is also called akisation, augmentation. Truncate cuts off the polyhedron at its vertices but leaves a portion of the original edges.[12] Zip is also called bitruncation .
4	${\displaystyle {\begin{bmatrix}1&1&1\\0&4&0\\0&2&0\end{bmatrix}}}$	Ortho: o = jj		Expand: e = aa
5	${\displaystyle {\begin{bmatrix}1&2&1\\0&5&0\\0&2&0\end{bmatrix}}}$	Gyro: g	gd = rgr	sd = rsr	Snub: s	Chiral operators. See Snub (geometry). Contrary to Hart,[3] gd is not the same as g: it is its chiral pair.[13]
6	${\displaystyle {\begin{bmatrix}1&1&1\\0&6&0\\0&4&0\end{bmatrix}}}$	Meta: m = kj		Bevel: b = ta

Seeds

Any polyhedron can serve as a seed, as long as the operations can be executed on it. Common seeds have been assigned a letter. The

can be referenced as J_n, for n=1..92.

All of the five Platonic solids can be generated from prismatic generators with zero to two operators:[14]

The regular Euclidean tilings can also be used as seeds:

• Q = Quadrille = Square tiling
• H = Hextille = Hexagonal tiling = dΔ
• Δ = Deltille = Triangular tiling = dH

Extended operations

These are operations created after Conway's original set. Note that many more operations exist than have been named; just because an operation is not here does not mean it does not exist (or is not an LSP or LOPSP). To simplify, only irreducible operators are included in this list: others can be created by composing operators together.

Irreducible extended operators

Edge factor	Matrix ${\displaystyle \mathbf {M} _{x}}$	x	xd	dx	dxd	Notes
4	${\displaystyle {\begin{bmatrix}1&2&0\\0&4&0\\0&1&1\end{bmatrix}}}$	Chamfer: c	cd = du	dc = ud	Subdivide: u	Chamfer is the join-form of l. See Chamfer (geometry).
5	${\displaystyle {\begin{bmatrix}1&2&0\\0&5&0\\0&2&1\end{bmatrix}}}$	Propeller: p	dp = pd		dpd = p	Chiral operators. The propeller operator was developed by George Hart.[15]
5	${\displaystyle {\begin{bmatrix}1&2&0\\0&5&0\\0&2&1\end{bmatrix}}}$	Loft: l	ld	dl	dld
6	${\displaystyle {\begin{bmatrix}1&3&0\\0&6&0\\0&2&1\end{bmatrix}}}$	Quinto: q	qd	dq	dqd
6	${\displaystyle {\begin{bmatrix}1&2&0\\0&6&0\\0&3&1\end{bmatrix}}}$	Join-lace: L0	L0d	dL0	dL0d	See below for explanation of join notation.
7	${\displaystyle {\begin{bmatrix}1&2&0\\0&7&0\\0&4&1\end{bmatrix}}}$	Lace: L	Ld	dL	dLd
7	${\displaystyle {\begin{bmatrix}1&2&1\\0&7&0\\0&4&0\end{bmatrix}}}$	Stake: K	Kd	dK	dKd
7	${\displaystyle {\begin{bmatrix}1&4&0\\0&7&0\\0&2&1\end{bmatrix}}}$	Whirl: w	wd = dv	vd = dw	Volute: v	Chiral operators.
8	${\displaystyle {\begin{bmatrix}1&2&1\\0&8&0\\0&5&0\end{bmatrix}}}$	Join-kis-kis: ${\displaystyle (kk)_{0}}$	${\displaystyle (kk)_{0}d}$	${\displaystyle d(kk)_{0}}$	${\displaystyle d(kk)_{0}d}$	Sometimes named J.[4] See below for explanation of join notation. The non-join-form, kk, is not irreducible.
10	${\displaystyle {\begin{bmatrix}1&3&1\\0&10&0\\0&6&0\end{bmatrix}}}$	Cross: X	Xd	dX	dXd

Indexed extended operations

A number of operators can be grouped together by some criteria, or have their behavior modified by an index.^[4] These are written as an operator with a subscript: x_n.

Augmentation

operations retain original edges. They may be applied to any independent subset of faces, or may be converted into a join-form by removing the original edges. Conway notation supports an optional index to these operators: 0 for the join-form, or 3 or higher for how many sides affected faces have. For example, k₄Y₄=O: taking a square-based pyramid and gluing another pyramid to the square base gives an octahedron.

Operator	k	l	L	K	(kk)
x
x0	k0 = j	l0 = c	L0	K0 = jk	${\displaystyle (kk)_{0}}$
Augmentation	Pyramid	Prism	Antiprism

The truncate operator t also has an index form t_n, indicating that only vertices of a certain degree are truncated. It is equivalent to dk_nd.

Some of the extended operators can be created in special cases with k_n and t_n operators. For example, a

, deD or oD, with its degree-5 vertices truncated.

Meta/Bevel

Meta adds vertices at the center and along the edges, while bevel adds faces at the center, seed vertices, and along the edges. The index is how many vertices or faces are added along the edges. Meta (in its non-indexed form) is also called

Meta/Bevel operators

n	Edge factor	Matrix ${\displaystyle \mathbf {M} _{x}}$	x	xd	dx	dxd
0	3	${\displaystyle {\begin{bmatrix}1&0&1\\0&3&0\\0&2&0\end{bmatrix}}}$	k = m0	n	z = b0	t
1	6	${\displaystyle {\begin{bmatrix}1&1&1\\0&6&0\\0&4&0\end{bmatrix}}}$	m = m1 = kj		b = b1 = ta
2	9	${\displaystyle {\begin{bmatrix}1&2&1\\0&9&0\\0&6&0\end{bmatrix}}}$	m2	m2d	b2	b2d
3	12	${\displaystyle {\begin{bmatrix}1&3&1\\0&12&0\\0&8&0\end{bmatrix}}}$	m3	m3d	b3	b3d
n	3n+3	${\displaystyle {\begin{bmatrix}1&n&1\\0&3n+3&0\\0&2n+2&0\end{bmatrix}}}$	mn	mnd	bn	bnd

Medial

Medial is like meta, except it does not add edges from the center to each seed vertex. The index 1 form is identical to Conway's ortho and expand operators: expand is also called cantellation and expansion. Note that o and e have their own indexed forms, described below. Also note that some implementations start indexing at 0 instead of 1.^[4]

Medial operators

n	Edge factor	Matrix ${\displaystyle \mathbf {M} _{x}}$	x	xd	dx	dxd
1	4	${\displaystyle {\begin{bmatrix}1&1&1\\0&4&0\\0&2&0\end{bmatrix}}}$	M1 = o = jj		e = aa
2	7	${\displaystyle {\begin{bmatrix}1&2&1\\0&7&0\\0&4&0\end{bmatrix}}}$	Medial: M = M2	Md	dM	dMd
n	3n+1	${\displaystyle {\begin{bmatrix}1&n&1\\0&3n+1&0\\0&2n&0\end{bmatrix}}}$	Mn	Mnd	dMn	dMnd

Goldberg-Coxeter

The Goldberg-Coxeter (GC) Conway operators are two infinite families of operators that are an extension of the

for formulas.

The two families are the triangular GC family, c_a,b and u_a,b, and the quadrilateral GC family, e_a,b and o_a,b. Both the GC families are indexed by two integers ${\displaystyle a\geq 1}$ and ${\displaystyle b\geq 0}$. They possess many nice qualities:

• The indexes of the families have a relationship with certain
  Gaussian integers
  for the quadrilateral GC family.
• Operators in the x and dxd columns within the same family commute with each other.

The operators are divided into three classes (examples are written in terms of c but apply to all 4 operators):

• Class I: ${\displaystyle b=0}$. Achiral, preserves original edges. Can be written with the zero index suppressed, e.g. c_a,0 = c_a.
• Class II: ${\displaystyle a=b}$. Also achiral. Can be decomposed as c_a,a = c_ac_1,1
• Class III: All other operators. These are chiral, and c_a,b and c_b,a are the chiral pairs of each other.

Of the original Conway operations, the only ones that do not fall into the GC family are g and s (gyro and snub). Meta and bevel (m and b) can be expressed in terms of one operator from the triangular family and one from the quadrilateral family.

Triangular

Triangular Goldberg-Coxeter operators

a	b	Class	Edge factor T = a2 + ab + b2	Matrix ${\displaystyle \mathbf {M} _{x}}$	Master triangle	x	xd	dx	dxd
1	0	I	1	${\displaystyle {\begin{bmatrix}1&0&0\\0&1&0\\0&0&1\end{bmatrix}}}$		u1 = S	d		c1 = S
2	0	I	4	${\displaystyle {\begin{bmatrix}1&1&0\\0&4&0\\0&2&1\end{bmatrix}}}$		u2 = u	dc	du	c2 = c
3	0	I	9	${\displaystyle {\begin{bmatrix}1&2&1\\0&9&0\\0&6&0\end{bmatrix}}}$		u3 = nn	nk	zt	c3 = zz
4	0	I	16	${\displaystyle {\begin{bmatrix}1&5&0\\0&16&0\\0&10&1\end{bmatrix}}}$		u4 = uu	uud = dcc	duu = ccd	c4 = cc
5	0	I	25	${\displaystyle {\begin{bmatrix}1&8&0\\0&25&0\\0&16&1\end{bmatrix}}}$		u5	u5d = dc5	du5 = c5d	c5
6	0	I	36	${\displaystyle {\begin{bmatrix}1&11&1\\0&36&0\\0&24&0\end{bmatrix}}}$		u6 = unn	unk	czt	u6 = czz
7	0	I	49	${\displaystyle {\begin{bmatrix}1&16&0\\0&49&0\\0&32&1\end{bmatrix}}}$		u7 = u2,1u1,2 = vrv	vrvd = dwrw	dvrv = wrwd	c7 = c2,1c1,2 = wrw
8	0	I	64	${\displaystyle {\begin{bmatrix}1&21&0\\0&64&0\\0&42&1\end{bmatrix}}}$		u8 = u3	u3d = dc3	du3 = c3d	c8 = c3
9	0	I	81	${\displaystyle {\begin{bmatrix}1&26&1\\0&81&0\\0&54&0\end{bmatrix}}}$		u9 = n4	n3k = kz3	tn3 = z3t	c9 = z4
1	1	II	3	${\displaystyle {\begin{bmatrix}1&0&1\\0&3&0\\0&2&0\end{bmatrix}}}$		u1,1 = n	k	t	c1,1 = z
2	1	III	7	${\displaystyle {\begin{bmatrix}1&2&0\\0&7&0\\0&4&1\end{bmatrix}}}$		v = u2,1	vd = dw	dv = wd	w = c2,1
3	1	III	13	${\displaystyle {\begin{bmatrix}1&4&0\\0&13&0\\0&8&1\end{bmatrix}}}$		u3,1	u3,1d = dc3,1	du3,1 = c3,1d	c3,1
3	2	III	19	${\displaystyle {\begin{bmatrix}1&6&0\\0&19&0\\0&12&1\end{bmatrix}}}$		u3,2	u3,2d = dc3,2	du3,2 = c3,2d	c3,2
4	3	III	37	${\displaystyle {\begin{bmatrix}1&12&0\\0&37&0\\0&24&1\end{bmatrix}}}$		u4,3	u4,3d = dc4,3	du4,3 = c4,3d	c4,3
5	4	III	61	${\displaystyle {\begin{bmatrix}1&20&0\\0&61&0\\0&40&1\end{bmatrix}}}$		u5,4	u5,4d = dc5,4	du5,4 = c5,4d	c5,4
6	5	III	91	${\displaystyle {\begin{bmatrix}1&30&0\\0&91&0\\0&60&1\end{bmatrix}}}$		u6,5 = u1,2u1,3	u6,5d = dc6,5	du6,5 = c6,5d	c6,5=c1,2c1,3
7	6	III	127	${\displaystyle {\begin{bmatrix}1&42&0\\0&127&0\\0&84&1\end{bmatrix}}}$		u7,6	u7,6d = dc7,6	du7,6 = c7,6d	c7,6
8	7	III	169	${\displaystyle {\begin{bmatrix}1&56&0\\0&169&0\\0&112&1\end{bmatrix}}}$		u8,7 = u3,12	u8,7d = dc8,7	du8,7 = c8,7d	c8,7 = c3,12
9	8	III	217	${\displaystyle {\begin{bmatrix}1&72&0\\0&217&0\\0&144&1\end{bmatrix}}}$		u9,8 = u2,1u5,1	u9,8d = dc9,8	du9,8 = c9,8d	c9,8 = c2,1c5,1
${\displaystyle a\equiv b}$${\displaystyle \ (\mathrm {mod} \ 3)}$		I, II, or III	${\displaystyle T\equiv 0\ }$${\displaystyle (\mathrm {mod} \ 3)}$	${\displaystyle {\begin{bmatrix}1&{\frac {T}{3}}-1&1\\0&T&0\\0&{\frac {2}{3}}T&0\end{bmatrix}}}$	...	ua,b	ua,bd = dca,b	dua,b = ca,bd	ca,b
${\displaystyle a\not \equiv b}$${\displaystyle \ (\mathrm {mod} \ 3)}$		I or III	${\displaystyle T\equiv 1}$${\displaystyle \ (\mathrm {mod} \ 3)}$	${\displaystyle {\begin{bmatrix}1&{\frac {T-1}{3}}&0\\0&T&0\\0&2{\frac {T-1}{3}}&1\end{bmatrix}}}$	...	ua,b	ua,bd = dca,b	dua,b = ca,bd	ca,b

By basic number theory, for any values of a and b, ${\displaystyle T\not \equiv 2\ (\mathrm {mod} \ 3)}$.

Quadrilateral

Quadrilateral Goldberg-Coxeter operators

a	b	Class	Edge factor T = a2 + b2	Matrix ${\displaystyle \mathbf {M} _{x}}$	Master square	x	xd	dx	dxd
1	0	I	1	${\displaystyle {\begin{bmatrix}1&0&0\\0&1&0\\0&0&1\end{bmatrix}}}$		o1 = S	e1 = d		o1 = dd = S
2	0	I	4	${\displaystyle {\begin{bmatrix}1&1&1\\0&4&0\\0&2&0\end{bmatrix}}}$		o2 = o = j2		e2 = e = a2
3	0	I	9	${\displaystyle {\begin{bmatrix}1&4&0\\0&9&0\\0&4&1\end{bmatrix}}}$		o3	e3		o3
4	0	I	16	${\displaystyle {\begin{bmatrix}1&7&1\\0&16&0\\0&8&0\end{bmatrix}}}$		o4 = oo = j4		e4 = ee = a4
5	0	I	25	${\displaystyle {\begin{bmatrix}1&12&0\\0&25&0\\0&12&1\end{bmatrix}}}$		o5 = o2,1o1,2 = prp	e5 = e2,1e1,2		o5= dprpd
6	0	I	36	${\displaystyle {\begin{bmatrix}1&17&1\\0&36&0\\0&18&0\end{bmatrix}}}$		o6 = o2o3		e6 = e2e3
7	0	I	49	${\displaystyle {\begin{bmatrix}1&24&0\\0&49&0\\0&24&1\end{bmatrix}}}$		o7	e7		o7
8	0	I	64	${\displaystyle {\begin{bmatrix}1&31&1\\0&64&0\\0&32&0\end{bmatrix}}}$		o8 = o3 = j6		e8 = e3 = a6
9	0	I	81	${\displaystyle {\begin{bmatrix}1&40&0\\0&81&0\\0&40&1\end{bmatrix}}}$		o9 = o32	e9 = e32		o9
10	0	I	100	${\displaystyle {\begin{bmatrix}1&49&1\\0&100&0\\0&50&0\end{bmatrix}}}$		o10 = oo2,1o1,2		e10 = ee2,1e1,2
1	1	II	2	${\displaystyle {\begin{bmatrix}1&0&1\\0&2&0\\0&1&0\end{bmatrix}}}$		o1,1 = j		e1,1 = a
2	2	II	8	${\displaystyle {\begin{bmatrix}1&3&1\\0&8&0\\0&4&0\end{bmatrix}}}$		o2,2 = j3		e2,2 = a3
1	2	III	5	${\displaystyle {\begin{bmatrix}1&2&0\\0&5&0\\0&2&1\end{bmatrix}}}$		o1,2 = p	e1,2 = dp = pd		p
${\displaystyle a\equiv b}$${\displaystyle \ (\mathrm {mod} \ 2)}$		I, II, or III	T even	${\displaystyle {\begin{bmatrix}1&{\frac {T}{2}}-1&1\\0&T&0\\0&{\frac {T}{2}}&0\end{bmatrix}}}$	...	oa,b		ea,b
${\displaystyle a\not \equiv b}$${\displaystyle \ (\mathrm {mod} \ 2)}$		I or III	T odd	${\displaystyle {\begin{bmatrix}1&{\frac {T-1}{2}}&0\\0&T&0\\0&{\frac {T-1}{2}}&1\end{bmatrix}}}$	...	oa,b	ea,b		oa,b

Examples

Archimedean and Catalan solids

Conway's original set of operators can create all of the

as seeds. (Note that the r operator is not necessary to create both chiral forms.)

• Archimedean
• 
  Truncated tetrahedron
  tT
• 
  Cuboctahedron
  aC = aO = eT
• 
  Truncated cube
  tC
• 
  Truncated octahedron
  tO = bT
• 
  Rhombicuboctahedron
  eC = eO
• 
  truncated cuboctahedron
  bC = bO
• 
  snub cube
  sC = sO
• 
  icosidodecahedron
  aD = aI
• 
  truncated dodecahedron
  tD
• 
  truncated icosahedron
  tI
• 
  rhombicosidodeca­hedron
  eD = eI
• 
  truncated icosidodecahedron
  bD = bI
• 
  snub dodecahedron
  sD = sI

• Catalan
• 
  Triakis tetrahedron
  kT
• 
  Rhombic dodecahedron
  jC = jO = oT
• 
  Triakis octahedron
  kO
• 
  Tetrakis hexahedron
  kC = mT
• 
  Deltoidal icositetrahedron
  oC = oO
• 
  Disdyakis dodecahedron
  mC = mO
• 
  Pentagonal icositetrahedron
  gC = gO
• 
  Rhombic triacontahedron
  jD = jI
• 
  Triakis icosahedron
  kI
• 
  Pentakis dodecahedron
  kD
• 
  Deltoidal hexecontahedron
  oD = oI
• 
  Disdyakis triacontahedron
  mD = mI
• 
  Pentagonal hexecontahedron
  gD = gI

Composite operators

The

.

• 
  tI
• 
  atI
• 
  ttI
• 
  ztI = ttD
• 
  etI
• 
  btI
• 
  stI

• Duals
• 
  dtI = nI = kD
• 
  jtI
• 
  ntI = kkD
• 
  ktI
• 
  otI
• 
  mtI
• 
  gtI

On the plane

Each of the

Q, H, and Δ.

• 
  Square tiling
  Q = dQ = aQ = eQ
  = jQ = oQ
• 
  Truncated square tiling
  tQ = bQ
• 
  Tetrakis square tiling
  kQ = mQ
• 
  Snub square tiling
  sQ
• 
  Cairo pentagonal tiling
  gQ

• 
  Hexagonal tiling
  H = dΔ = tΔ
• 
  Trihexagonal tiling
  aH = aΔ
• 
  Truncated hexagonal tiling
  tH
• 
  Rhombitrihexagonal tiling
  eH = eΔ
• 
  Truncated trihexagonal tiling
  bH = bΔ
• 
  Snub trihexagonal tiling
  sH = sΔ

• 
  Triangle tiling

  
  Δ = dH = kH
• 
  Rhombille tiling
  jΔ = jH
• 
  Triakis triangular tiling

  
  kΔ
• 
  Deltoidal trihexagonal tiling

  
  oΔ = oH
• 
  Kisrhombille tiling

  
  mΔ = mH
• 
  Floret pentagonal tiling

  
  gΔ = gH

On a torus

Conway operators can also be applied to

and polyhedra with multiple holes.

• 
  A 1x1 regular square torus, {4,4}_1,0
• 
  A regular 4x4 square torus, {4,4}_4,0
• 
  tQ24×12 projected to torus
• 
  taQ24×12 projected to torus
• 
  actQ24×8 projected to torus
• 
  tH24×12 projected to torus
• 
  taH24×8 projected to torus
• 
  kH24×12 projected to torus

See also

• Symmetrohedron
• Zonohedron
• Schläfli symbol

References

External links

• polyHédronisme: generates polyhedra in HTML5 canvas, taking Conway notation as input