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		<summary type="html">&lt;p&gt;70.210.13.113: /* Markers */&lt;/p&gt;
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&lt;div&gt;Many branches of mathematics study objects of a given type and prove a [[classification theorem]]. A common theme is that the classification results in a number of series of objects and a finite number of exceptions that don&#039;t fit into any series. These are known as &#039;&#039;&#039;exceptional objects&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
Frequently these exceptional objects play a further and important role in the subject. Surprisingly, the exceptional objects in one branch of mathematics are often related to the exceptional objects in others.&lt;br /&gt;
&lt;br /&gt;
A related phenomenon is [[exceptional isomorphism]], when two series are in general different, but agree for some small values.&lt;br /&gt;
&lt;br /&gt;
== Regular polytopes ==&lt;br /&gt;
{{Main|Regular polytope}}&lt;br /&gt;
The prototypical examples of exceptional objects arise when we classify the [[regular polytope]]s. In 2 dimensions we have a series of [[regular polygon|regular &#039;&#039;n&#039;&#039;-gons]] for &#039;&#039;n&#039;&#039;&amp;amp;nbsp;≥&amp;amp;nbsp;3. In every dimension above 2 we find analogues of the cube, tetrahedron and octahedron. In 3 dimensions we find two more regular polyhedra – the [[dodecahedron]] (12-cell) and the [[icosahedron]] (20-cell) – making 5 [[Platonic solids]]. In 4 dimensions we have a total of 6 [[Convex regular 4-polytope|regular polytopes]] including the [[120-cell]], the [[600-cell]] and the [[24-cell]]. There are no other regular polytopes; in higher dimensions the only regular polytopes are of the [[hypercube]], [[simplex]], [[orthoplex]] series. So we have three series and 5 exceptional polytopes.&lt;br /&gt;
&lt;br /&gt;
The pattern is similar if non-convex polytopes are included.  In two dimensions there is a [[regular star polygon]] for every [[rational number]] &#039;&#039;p&#039;&#039;/&#039;&#039;q&#039;&#039;&amp;amp;nbsp;&amp;gt;&amp;amp;nbsp;2.  In three dimensions there are four [[Kepler–Poinsot polyhedron|Kepler–Poinsot polyhedra]], and in four dimensions ten [[Schläfli–Hess polychoron|Schläfli–Hess polychora]]; in higher dimensions there are no non-convex regular figures.&lt;br /&gt;
&lt;br /&gt;
These can be generalized to [[tessellation]]s of other spaces, especially [[uniform tessellation]]s, notably tilings of Euclidean space ([[honeycomb (geometry)|honeycombs]]), which have exceptional objects, and tilings of hyperbolic space. There are various exceptional objects in dimension below 6, but in dimension 6 and above the only regular polyhedra/tilings/hyperbolic tilings are the simplex, hypercube, cross-polytope, and hypercube lattice.&lt;br /&gt;
&lt;br /&gt;
=== Schwarz triangles ===&lt;br /&gt;
{{see|Schwarz triangle}}&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; align=right&lt;br /&gt;
|[[Image:Sphere symmetry group td.png|120px]]&amp;lt;BR&amp;gt;(3 3 2)&lt;br /&gt;
|[[Image:Sphere symmetry group oh.png|120px]]&amp;lt;BR&amp;gt;(4 3 2)&lt;br /&gt;
|[[Image:Sphere symmetry group ih.png|120px]]&amp;lt;BR&amp;gt;(5 3 2)&lt;br /&gt;
|-&lt;br /&gt;
|[[Image:Tile 3,6.svg|120px]]&amp;lt;BR&amp;gt;(3 3 3)&lt;br /&gt;
|[[Image:Tile V488 bicolor.svg|120px]]&amp;lt;BR&amp;gt;(4 4 2)&lt;br /&gt;
|[[Image:Tile V46b.svg|120px]]&amp;lt;BR&amp;gt;(6 3 2)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Related to tilings and the regular polyhedra, there are exceptional [[Schwarz triangle]]s (triangles that tile the sphere, or more generally Euclidean plane or hyperbolic plane via their [[triangle group]] of reflections in their edges), particularly the [[Möbius triangle]]s. In the sphere there are 3 Möbius triangles (and 1 1-parameter family), corresponding to the 3 exceptional Platonic solid groups, while in the Euclidean plane there are 3 Möbius triangles, corresponding to the 3 special triangles: 60-60-60 ([[equilateral triangle|equilateral]]), [[45-45-90]] (isosceles right), and [[30-60-90]]. There are additional exceptional Schwarz triangles in the sphere and Euclidean plane. By contrast, in the hyperbolic plane there is a 3-parameter family of Möbius triangles, and none exceptional.&lt;br /&gt;
&lt;br /&gt;
== Finite simple groups ==&lt;br /&gt;
{{Main|Sporadic group}}&lt;br /&gt;
[[File:Finitesubgroups.svg|thumb|The relations between the sporadic groups, most being related to the monster.]]&lt;br /&gt;
&lt;br /&gt;
The finite simple groups have been [[Classification of finite simple groups|classified]] into a number of series as well as 26 [[sporadic groups]]. Of these, 20 are subgroups or subquotients of the [[monster group]], referred to as the &amp;quot;Happy Family&amp;quot;, while 6 are not, and are referred to as &amp;quot;[[Pariah group|pariahs]]&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
Several of the sporadic groups are related to the Leech lattice, most notably the Conway group Co&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, which is the automorphism group of the Leech lattice, quotiented out by its center.&lt;br /&gt;
&lt;br /&gt;
== Division algebras ==&lt;br /&gt;
&lt;br /&gt;
There are only three associative [[division algebras]] over the reals - the [[real numbers]], the [[complex numbers]] and the [[quaternions]]. The only non-associative division algebra is the algebra of [[octonions]]. The octonions are connected to a wide variety of exceptional objects. For example the exceptional formally real [[Jordan algebra]] is the [[Albert algebra]] of 3 by 3 self-adjoint matrices over the octonions.&lt;br /&gt;
&lt;br /&gt;
== Simple Lie groups ==&lt;br /&gt;
&lt;br /&gt;
The [[simple Lie group]]s form a number of series ([[classical Lie group]]s) labelled A, B, C and D. In addition we have the exceptional groups [[G2 (mathematics)|G&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]] (the automorphism group of the octonions), [[F4 (mathematics)|F&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;]], [[E6 (mathematics)|E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;]], [[E7 (mathematics)|E&amp;lt;sub&amp;gt;7&amp;lt;/sub&amp;gt;]], [[E8 (mathematics)|E&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt;]]. These last four groups can be viewed as the symmetry groups of projective planes over &#039;&#039;&#039;O&#039;&#039;&#039;, &#039;&#039;&#039;C&#039;&#039;&#039;⊗&#039;&#039;&#039;O&#039;&#039;&#039;, &#039;&#039;&#039;H&#039;&#039;&#039;⊗&#039;&#039;&#039;O&#039;&#039;&#039; and &#039;&#039;&#039;O&#039;&#039;&#039;⊗&#039;&#039;&#039;O&#039;&#039;&#039; respectively, where &#039;&#039;&#039;O&#039;&#039;&#039; is the octonions and the tensor products are over the reals.&lt;br /&gt;
&lt;br /&gt;
The classification of Lie groups corresponds to the classification of [[root systems]] and so the exceptional Lie groups correspond to exceptional root systems and exceptional [[Dynkin diagram]]s.&lt;br /&gt;
&lt;br /&gt;
== Supersymmetric algebras ==&lt;br /&gt;
There are a few exceptional objects with [[supersymmetry]]. The [[Lie superalgebra]]s &#039;&#039;&#039;G(3)&#039;&#039;&#039; in 31 dimensions and &#039;&#039;&#039;F(4)&#039;&#039;&#039; in 40 dimensions and the Jordan superalgebras &#039;&#039;&#039;K&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039; and &#039;&#039;&#039;K&amp;lt;sub&amp;gt;10&amp;lt;/sub&amp;gt;&#039;&#039;&#039; being the main finite dimensional examples.&lt;br /&gt;
&lt;br /&gt;
== Unimodular lattices ==&lt;br /&gt;
&lt;br /&gt;
Up to isometry there is only one even [[unimodular lattice]] in 15 dimensions or less &amp;amp;mdash; the [[E8 lattice|E&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt; lattice]]. Up to dimension [[24 (number)|24]] there is only one even unimodular lattice with no [[root system|roots]], the [[Leech lattice]]. Three of the sporadic simple groups were discovered by Conway while investigating the automorphism group of the Leech lattice. For example [[Conway group|Co&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;]] is the automorphism group itself modulo ±1. The groups [[Conway group|Co&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]] and [[Conway group|Co&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]], as well as a number of other sporadic groups, arise as stabilisers of various subsets of the Leech lattice.&lt;br /&gt;
&lt;br /&gt;
== Codes ==&lt;br /&gt;
&lt;br /&gt;
Some [[Error-correcting code|codes]] also stand out as exceptional objects, in particular the perfect binary Golay code which is closely related to the Leech lattice. The Mathieu group &amp;lt;math&amp;gt;M_{24}&amp;lt;/math&amp;gt;, one of the sporadic simple groups, is the group of automorphisms of the [[binary Golay code|extended binary Golay code]] and four more of the sporadic simple groups arise as various types of stabilizer subgroup of &amp;lt;math&amp;gt;M_{24}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Block designs ==&lt;br /&gt;
&lt;br /&gt;
An exceptional [[block design]] is the [[Steiner system]] S(5,8,24) whose automorphism group is the sporadic simple [[Mathieu group]] &amp;lt;math&amp;gt;M_{24}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Snarks ==&lt;br /&gt;
&lt;br /&gt;
In [[graph theory]], we can have [[snark (graph theory)|snark]]s.&lt;br /&gt;
&lt;br /&gt;
== Outer automorphisms ==&lt;br /&gt;
Certain families of groups generically have a certain [[outer automorphism group]], but in particular cases they have other, exceptional outer automorphisms.&lt;br /&gt;
&lt;br /&gt;
Among families of finite simple groups, the only example&amp;lt;ref&amp;gt;ATLAS p. xvi&amp;lt;/ref&amp;gt; is in the [[automorphisms of the symmetric and alternating groups]]: for &amp;lt;math&amp;gt;n \geq 3, n \neq 6&amp;lt;/math&amp;gt; the [[alternating group]] &amp;lt;math&amp;gt;A_n&amp;lt;/math&amp;gt; has one outer automorphism (corresponding to conjugation by an odd element of &amp;lt;math&amp;gt;S_n&amp;lt;/math&amp;gt;) and the [[symmetric group]] &amp;lt;math&amp;gt;S_n&amp;lt;/math&amp;gt; has no outer automorphisms. However, for &amp;lt;math&amp;gt;n=6,&amp;lt;/math&amp;gt; there is an [[Automorphisms of the symmetric and alternating groups#exceptional outer automorphism|exceptional outer automorphism]] of &amp;lt;math&amp;gt;S_6&amp;lt;/math&amp;gt; (of order 2), and correspondingly, the outer automorphism group of &amp;lt;math&amp;gt;A_6&amp;lt;/math&amp;gt; is not &amp;lt;math&amp;gt;C_2&amp;lt;/math&amp;gt; (the group of order 2) but rather &amp;lt;math&amp;gt;C_2 \times C_2&amp;lt;/math&amp;gt; (the [[Klein four-group]]).&lt;br /&gt;
&lt;br /&gt;
If one instead considers A&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; as the (isomorphic) [[projective special linear group]] PSL(2,9), then the outer automorphism is not exceptional; thus the exceptionalness can be seen as due to the [[exceptional isomorphism]] &amp;lt;math&amp;gt;A_6 \cong \operatorname{PSL}(2,9).&amp;lt;/math&amp;gt; This exceptional outer automorphism is realized inside of the Mathieu group M&amp;lt;sub&amp;gt;12&amp;lt;/sub&amp;gt; and similarly, M&amp;lt;sub&amp;gt;12&amp;lt;/sub&amp;gt; acts on a set of 12 elements in 2 different ways.&lt;br /&gt;
&lt;br /&gt;
[[File:Dynkin diagram D4.png|thumb|The symmetries of the Dynkin diagram D&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; correspond to the [[outer automorphism]]s of Spin(8) in triality]]&lt;br /&gt;
Among [[Lie groups]], the [[spin group]] Spin(8) has an exceptionally large outer automorphism group (namely &amp;lt;math&amp;gt;S_3&amp;lt;/math&amp;gt;), which corresponds to the exceptional symmetries of the [[Dynkin diagram]] D&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;. This phenomenon is referred to as &#039;&#039;[[triality]].&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The exceptional symmetry of the D&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; diagram also gives rise to the [[Steinberg group (Lie theory)|Steinberg groups]].&lt;br /&gt;
&lt;br /&gt;
== Algebraic topology ==&lt;br /&gt;
{{Expand section|date=January 2010}}&lt;br /&gt;
The five or six (depending on the status of &#039;&#039;n&#039;&#039;=126) (framed [[cobordism class]]es of) manifolds of [[Kervaire invariant]] one, which exist in dimension &amp;lt;math&amp;gt;n=2^k-2&amp;lt;/math&amp;gt; for &amp;lt;math&amp;gt;n=2, 6, 14, 30, 62,&amp;lt;/math&amp;gt; and possibly 126, but no higher, are exceptional objects related to [[exotic sphere]]s. It is conjectured that these are related to the [[Rosenfeld projective plane]]s (over octonions and related) and exceptional Lie algebras, due to similarities of dimensions, but no connection has been established.&lt;br /&gt;
&lt;br /&gt;
== Connections ==&lt;br /&gt;
Numerous connections have been observed between some, though not all, of these exceptional objects. Most common are objects related to [[8 (number)|8]] and [[24 (number)|24]] dimensions, noting that 24&amp;amp;nbsp;=&amp;amp;nbsp;8&amp;amp;nbsp;·&amp;amp;nbsp;3.  By contrast, the [[pariah group]]s stand apart, as the name suggests.&lt;br /&gt;
&lt;br /&gt;
=== 8 dimensions ===&lt;br /&gt;
* The octonions are 8-dimensional.&lt;br /&gt;
* The [[E8 lattice|E&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt; lattice]] can be realized as the integral octonions (up to a scale factor).&lt;br /&gt;
* The exceptional Lie groups can be seen as symmetries of the octonions and structures derived from the octonions; further, the E&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt; algebra is related to the E&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt; lattice, as the notation implies (the lattice is generated by the root system of the algebra).&lt;br /&gt;
* Triality occurs for Spin(8), which also connects to 8&amp;amp;nbsp;·&amp;amp;nbsp;3 &amp;amp;nbsp;=&amp;amp;nbsp;24.&lt;br /&gt;
&lt;br /&gt;
=== 24 dimensions ===&lt;br /&gt;
* The Leech lattice is 24-dimensional.&lt;br /&gt;
* Most sporadic simple groups can be related to the Leech lattice, or more broadly the monster.&lt;br /&gt;
* The exceptional [[Jordan algebra]] has a representation in terms of 24&amp;amp;times;24 real matrices together with the Jordan product rule.&lt;br /&gt;
&lt;br /&gt;
=== Other phenomena ===&lt;br /&gt;
These objects are connected to various other phenomena in math which may be considered surprising but not themselves &amp;quot;exceptional&amp;quot;. For example, in [[algebraic topology]], 8-fold real [[Bott periodicity]] can be seen as coming from the octonions. In the theory of [[modular forms]], the 24-dimensional nature of the Leech lattice underlies the presence of 24 in the formulas for the [[Dedekind eta function]] and the [[modular discriminant]], which connection is deepened by [[monstrous moonshine]], which related modular functions to the monster group.&lt;br /&gt;
&lt;br /&gt;
=== Physics ===&lt;br /&gt;
In [[string theory]] and superstring theory we often find that particular dimensions are singled out as a result of exceptional algebraic phenomena. For example, [[bosonic string theory]] requires a spacetime of dimension 26 which is directly related to the presence of 24 in the [[Dedekind eta function]]. Similarly, the possible dimensions of [[supergravity]] are related to the dimensions of the [[division algebras]].&lt;br /&gt;
&lt;br /&gt;
== Unexceptional objects ==&lt;br /&gt;
=== Pathologies ===&lt;br /&gt;
{{See also|Pathological (mathematics)}}&lt;br /&gt;
&amp;quot;Exceptional&amp;quot; object is reserved for objects that are unusual, meaning rare, the exception, not for &#039;&#039;unexpected&#039;&#039; or &#039;&#039;non-standard&#039;&#039; objects. These unexpected-but-typical (or common) phenomena are generally referred to as [[Pathological (mathematics)|pathological]], such as [[nowhere differentiable function]]s, or &amp;quot;exotic&amp;quot;, as in [[exotic sphere]]s – there are exotic spheres in arbitrarily high dimension (not only a finite set of exceptions), and in many dimensions most (differential structures on) spheres are exotic.&lt;br /&gt;
&lt;br /&gt;
=== Extremal objects ===&lt;br /&gt;
Exceptional objects must be distinguished from &#039;&#039;extremal&#039;&#039; objects: those that fall in a family and are the most extreme example by some measure are of interest, but not unusual in the way exceptional objects are. For example, the [[golden ratio]] &#039;&#039;φ&#039;&#039; has the simplest [[continued fraction]] approximation, and accordingly is most difficult to [[Diophantine approximation|approximate by rationals]]; however, it is but one of infinitely many such quadratic numbers (continued fractions).&lt;br /&gt;
&lt;br /&gt;
Similarly, the (2,3,7) [[Schwarz triangle]] is the smallest hyperbolic Schwarz triangle, and the associated [[(2,3,7) triangle group]] is of particular interest, being the universal [[Hurwitz group]], and thus being associated with the [[Hurwitz curve]]s, the maximally symmetric algebraic curves. However, it falls in a family of such triangles ((2,4,7), (2,3,8), (3,3,7), etc.), and while the smallest, is not exceptional or unlike the others.&lt;br /&gt;
&lt;br /&gt;
== Connections ==&lt;br /&gt;
Many of the exceptional objects in mathematics and physics have been found to be connected to each other. Conjectures such as the [[Monstrous moonshine]] conjectures show how, for example, the [[Monster group]] is connected to [[String Theory]]. The theory of [[modular forms]] shows how the E8 is connected to the Monster group. Other interesting connections include how the [[Leech lattice]] is connected via the [[Golay code]] to the adjacency matrix of the [[dodecahedron]] (another exceptional object). Below is a [[mind map]] showing how some of the exceptional objects in mathematical physics are related. &lt;br /&gt;
&lt;br /&gt;
[[File:Exceptionalmindmap.png|600px]]&lt;br /&gt;
&lt;br /&gt;
The connections can partly be explained by thinking of the algebras as a tower of lattice [[vertex operator algebra]]s. It just so happens that the vertex algebras at the bottom are so simple that they are isomorphic to familiar non-vertex algebras. Thus the connections can be seen simply as the consequence of some lattices being sub-lattices of others.&lt;br /&gt;
&lt;br /&gt;
=== Supersymmetries ===&lt;br /&gt;
The [[Jordan superalgebra]]s are a parallel set of exceptional objects with [[supersymmetry]]. These are the [[Lie superalgebra]]s which are related to Lorentzian lattices. This subject is less developed so the connections between the objects is less developed. There are new conjectures parallel to the [[Monstrous moonshine]] conjectures for these super-objects involving different sporadic groups.&lt;br /&gt;
&lt;br /&gt;
[[File:supermindmap.png|550px]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Exceptional isomorphism]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
{{refbegin}}&lt;br /&gt;
* {{citation&lt;br /&gt;
|last=Stillwell&lt;br /&gt;
|first=John&lt;br /&gt;
|jstor=2589218&lt;br /&gt;
|title=Exceptional Objects&lt;br /&gt;
|journal=[[American Mathematical Monthly]]&lt;br /&gt;
|date=November 1998&lt;br /&gt;
|pages=850–858&lt;br /&gt;
}}&lt;br /&gt;
* [[John Baez]] and [[John Huerta]], &#039;&#039;Division Algebras and Supersymmetry II&#039;&#039;. {{arxiv|1003.3436}}.&lt;br /&gt;
* [http://math.ucr.edu/home/baez/week106.html This Week&#039;s Finds in Mathematical Physics, Week 106], [[John Baez]]&lt;br /&gt;
* [http://math.ucr.edu/home/baez/platonic.html Platonic Solids in all Dimensions], [[John Baez]]&lt;br /&gt;
{{refend}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Mathematical terminology]]&lt;/div&gt;</summary>
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