Editing Leech lattice

{{Short description|24-dimensional repeating pattern of points}}
In [[mathematics]], the '''Leech lattice''' is an even [[unimodular lattice]] Λ<sub>24</sub> in 24-dimensional [[Euclidean space]], which is one of the best models for the [[kissing number problem]]. It was discovered by {{harvs|txt|authorlink=John Leech (mathematician)|first=John|last= Leech|year=1967}}. It may also have been discovered (but not published) by [[Ernst Witt]] in 1940.

==Characterization==

The Leech lattice Λ<sub>24</sub> is the unique lattice in 24-dimensional [[Euclidean space]], '''E'''<sup>24</sup>, with the following list of properties:

*It is [[unimodular lattice|unimodular]]; i.e., it can be generated by the columns of a certain 24&times;24 [[matrix (mathematics)|matrix]] with [[determinant]]&nbsp;1.
*It is even; i.e., the square of the length of each vector in Λ<sub>24</sub> is an even integer.
*The length of every non-zero vector in Λ<sub>24</sub> is at least 2.

The last condition is equivalent to the condition that unit balls centered at the points of Λ<sub>24</sub> do not overlap.  Each is tangent to 196,560 neighbors, and this is known to be the largest number of non-overlapping 24-dimensional unit balls that can [[kissing number|simultaneously touch a single unit ball]]. This arrangement of 196,560 unit balls centred about another unit ball is so efficient that there is no room to move any of the balls; this configuration, together with its mirror-image, is the ''only'' 24-dimensional arrangement where 196,560 unit balls simultaneously touch another. This property is also true in 1, 2 and 8 dimensions, with 2, 6 and 240 unit balls, respectively, based on the [[integer lattice]], [[hexagonal tiling]] and [[E8 lattice|E<sub>8</sub> lattice]], respectively.

It has no [[root system]] and in fact is the first [[unimodular lattice]] with no ''roots'' (vectors of norm less than 4), and therefore has a centre density of 1. By multiplying this value by the volume of a unit ball in 24 dimensions, <math>\tfrac{\pi^{12}}{12!}</math>, one can derive its absolute density.

{{harvtxt|Conway|1983}} showed that the Leech lattice is isometric  to the set of simple roots (or the [[Dynkin diagram]]) of the [[reflection group]] of the 26-dimensional even Lorentzian unimodular lattice [[II25,1|II<sub>25,1</sub>]]. By comparison, the Dynkin diagrams of II<sub>9,1</sub> and II<sub>17,1</sub> are finite.

==Applications==

The [[binary Golay code]], independently developed in 1949, is an application in [[coding theory]]. More specifically, it is an error-correcting code capable of correcting up to three errors in each 24-bit word, and detecting up to four. It was used to communicate with the [[Voyager probes]], as it is much more compact than the previously-used [[Hadamard code]].

[[Quantizer]]s, or [[analog-to-digital converter]]s, can use lattices to minimise the average [[root-mean-square]] error. Most quantizers are based on the one-dimensional [[integer lattice]], but using multi-dimensional lattices reduces the RMS error. The Leech lattice is a good solution to this problem, as the [[Voronoi cell]]s have a low [[second moment]].

The [[vertex algebra]] of the [[two-dimensional conformal field theory]] describing [[bosonic string theory]], compactified on the 24-dimensional [[quotient group|quotient]] [[torus]] '''R'''<sup>24</sup>/Λ<sub>24</sub> and [[orbifold]]ed by a two-element reflection group, provides an explicit construction of the [[Griess algebra]] that has the [[monster group]] as its automorphism group. This '''[[monster vertex algebra]]''' was also used to prove the [[monstrous moonshine]] conjectures.

==Constructions==

The Leech lattice can be constructed in a variety of ways. Like all lattices, it can be constructed by taking the [[integer|integral]] span of the columns of its [[generator matrix]], a 24&times;24 matrix with [[determinant]] 1.

{{hidden | Leech generator matrix |
A 24x24 generator (in row convention) for the Leech Lattice is given by the following matrix divided by <math>\sqrt{8}</math>:
 <nowiki>
 8 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 0 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 2 2 2 2 2 2 2 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 0 0 0 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 0 0 0 0 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 0 0 0 0 0 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0
 2 2 2 2 0 0 0 0 2 2 2 2 0 0 0 0 0 0 0 0 0 0 0 0
 4 0 0 0 0 0 0 0 0 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0
 2 2 0 0 2 2 0 0 2 2 0 0 2 2 0 0 0 0 0 0 0 0 0 0
 2 0 2 0 2 0 2 0 2 0 2 0 2 0 2 0 0 0 0 0 0 0 0 0
 2 0 0 2 2 0 0 2 2 0 0 2 2 0 0 2 0 0 0 0 0 0 0 0
 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 4 0 0 0 0 0 0 0
 2 0 2 0 2 0 0 2 2 2 0 0 0 0 0 0 2 2 0 0 0 0 0 0
 2 0 0 2 2 2 0 0 2 0 2 0 0 0 0 0 2 0 2 0 0 0 0 0
 2 2 0 0 2 0 2 0 2 0 0 2 0 0 0 0 2 0 0 2 0 0 0 0
 0 2 2 2 2 0 0 0 2 0 0 0 2 0 0 0 2 0 0 0 2 0 0 0
 0 0 0 0 0 0 0 0 2 2 0 0 2 2 0 0 2 2 0 0 2 2 0 0
 0 0 0 0 0 0 0 0 2 0 2 0 2 0 2 0 2 0 2 0 2 0 2 0
−3 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
</nowiki>
}}<ref>{{citation | zbl=0915.52003 | last1=Conway | first1=J.H. | author1-link=John Horton Conway | last2=Sloane | first2=N.J.A. | author2-link=Neil Sloane | others=With contributions by Bannai, E.; Borcherds, R. E.; Leech, J.; Norton, S. P.; Odlyzko, A. M.; Parker, R. A.; Queen, L.; Venkov, B. B. | title=Sphere packings, lattices and groups | edition=Third | series=Grundlehren der Mathematischen Wissenschaften | volume=290 | location=New York, NY | publisher=[[Springer-Verlag]] | isbn=978-0-387-98585-5 | mr=662447 | year=1999 | url-access=registration | url=https://archive.org/details/spherepackingsla0000conw_b8u0 }}</ref>

===Using the binary Golay code===

The Leech lattice can be explicitly constructed as the set of vectors of the form 2<sup>&minus;3/2</sup>(''a''<sub>1</sub>, ''a''<sub>2</sub>, ..., ''a''<sub>24</sub>) where the ''a''<sub>''i''</sub> are integers such that

:<math>a_1+a_2+\cdots+a_{24}\equiv 4a_1\equiv 4a_2\equiv\cdots\equiv4a_{24}\pmod 8</math>

and for each fixed residue class modulo 4, the 24 bit word, whose 1s correspond to the coordinates ''i'' such that ''a''<sub>''i''</sub> belongs to this residue class, is a word in the [[binary Golay code]]. The Golay code, together with the related Witt design, features in a construction for the 196560 minimal vectors in the Leech lattice.

Leech lattice (L mod 8) can be directly constructed by combination of the 3 following sets,

<math>L ~ = ~~ (4B + C)\otimes{1_{2^{12}}}  ~~ + ~~~  {1_{2^{24}}}\otimes 2G  ~~~ </math> ,      (<math>{1_{n}}</math> is a ones vector of size n),
* G - 24-bit Golay code
* B - Binary integer sequence
* C - [[Thue-Morse sequence|Thue-Morse Sequence]] or integer bit parity sum (that give chirality of the lattice)
<syntaxhighlight lang="c">
24-bit Golay  [2^12 codes]   24-bit integer[2^24 codes]   Parity   Leech Lattice [2^36 codes]
G =                          B =                          C =      L = (4B + C) ⊕ 2G
00000000 00000000 00000000   00000000 00000000 00000000   0        00000000 00000000 00000000
11111111 00000000 00000000   10000000 00000000 00000000   1        22222222 00000000 00000000
11110000 11110000 00000000   01000000 00000000 00000000   1        22220000 22220000 00000000
00001111 11110000 00000000   11000000 00000000 00000000   0        ...
11001100 11001100 00000000   00100000 00000000 00000000   1        51111111 11111111 11111111
00110011 11001100 00000000   10100000 00000000 00000000   0        73333333 11111111 11111111
00111100 00111100 00000000   01100000 00000000 00000000   0        ...
11000011 00111100 00000000   11100000 00000000 00000000   1        15111111 11111111 11111111
10101010 10101010 00000000   00010000 00000000 00000000   1        37333333 11111111 11111111
01010101 10101010 00000000   10010000 00000000 00000000   0        ...
01011010 01011010 00000000   01010000 00000000 00000000   0        44000000 00000000 00000000
10100101 01011010 00000000   11010000 00000000 00000000   1        66222222 00000000 00000000
...                          ...                          ...      ...
11111111 11111111 11111111   11111111 11111111 11111111   0        66666666 66666666 66666666
</syntaxhighlight>

===Using the Lorentzian lattice II<sub>25,1</sub>===

The Leech lattice can also be constructed as <math>w^\perp/w</math> where ''w'' is the Weyl vector:

:<math>(0,1,2,3,\dots,22,23,24; 70)</math>

in the 26-dimensional even Lorentzian [[unimodular lattice]] [[II25,1|II<sub>25,1</sub>]]. The existence of such an integral vector of Lorentzian norm zero relies on the fact that 1<sup>2</sup> + 2<sup>2</sup> + ... + 24<sup>2</sup> is a [[square number|perfect square]] (in fact 70<sup>2</sup>); the [[24 (number)|number 24]] is the only integer bigger than 1 with this property (see [[cannonball problem]]). This was conjectured by [[Édouard Lucas]], but the proof came much later, based on [[elliptic functions]].

The vector
<math>(0,1,2,3,\dots,22,23,24)</math>
in this construction is really the [[Weyl vector]] of the even sublattice ''D''<sub>24</sub> of the odd unimodular lattice ''I''<sup>25</sup>. More generally, if ''L'' is any positive definite unimodular lattice of dimension 25 with at least 4 vectors of norm 1, then the Weyl vector of its norm 2 roots has integral length, and there is a similar construction of the Leech lattice using ''L'' and this Weyl vector.

===Based on other lattices===

{{harvtxt|Conway|Sloane|1982}} described another 23 constructions for the Leech lattice, each based on a [[Niemeier lattice]]. It can also be constructed by using three copies of the [[E8 lattice]], in the same way that the binary Golay code can be constructed using three copies of the extended [[Hamming code]], H<sub>8</sub>. This construction is known as the '''Turyn''' construction of the Leech lattice.

===As a laminated lattice===

Starting with a single point, Λ<sub>0</sub>, one can stack copies of the lattice Λ<sub>n</sub> to form an (''n''&nbsp;+&nbsp;1)-dimensional lattice, Λ<sub>''n''+1</sub>, without reducing the minimal distance between points. Λ<sub>1</sub> corresponds to the [[integer lattice]], Λ<sub>2</sub> is to the [[hexagonal lattice]], and Λ<sub>3</sub> is the [[face-centered cubic]] packing. {{harvtxt|Conway|Sloane|1982b}} showed that the Leech lattice is the unique laminated lattice in 24 dimensions.

===As a complex lattice===

The Leech lattice is also a 12-dimensional lattice over the [[Eisenstein integers]]. This is known as the '''complex Leech lattice''', and is isomorphic to the 24-dimensional real Leech lattice. In the complex construction of the Leech lattice, the [[binary Golay code]] is replaced with the [[ternary Golay code]], and the [[Mathieu group M24|Mathieu group ''M''<sub>24</sub>]] is replaced with the [[Mathieu group M12|Mathieu group ''M''<sub>12</sub>]]. The ''E''<sub>6</sub> lattice, ''E''<sub>8</sub> lattice and [[Coxeter&ndash;Todd lattice]] also have constructions as complex lattices, over either the Eisenstein or [[Gaussian integers]].

===Using the icosian ring===

The Leech lattice can also be constructed using the ring of [[icosian]]s. The icosian ring is abstractly isomorphic to the [[E8 lattice]], three copies of which can be used to construct the Leech lattice using the Turyn construction.

===Witt's construction===

In 1972 Witt gave the following construction, which he said he found in 1940, on January 28. Suppose that ''H'' is an ''n'' by ''n'' [[Hadamard matrix]], where ''n''=4''ab''. Then the matrix <math>\begin{pmatrix} Ia&H/2\\H/2&Ib\end{pmatrix}</math> defines a bilinear form in 2''n'' dimensions, whose kernel has ''n'' dimensions. The quotient by this kernel is a nonsingular bilinear form taking values in (1/2)'''Z'''. It has 3 sublattices of index 2 that are integral bilinear forms. Witt obtained the Leech lattice as one of these three sublattices by taking ''a''=2, ''b''=3, and taking ''H'' to be the 24 by 24 matrix (indexed by '''Z'''/23'''Z''' ∪ ∞) with entries Χ(''m''+''n'') where Χ(∞)=1, Χ(0)=−1, Χ(''n'')=is the quadratic residue symbol mod 23 for nonzero ''n''. This matrix ''H'' is a [[Paley matrix]] with some insignificant sign changes.

===Using a Paley matrix===

{{harvtxt|Chapman|2001}} described a construction using a
[[Hadamard matrix#Skew Hadamard matrices|skew Hadamard matrix]] of [[Paley matrix|Paley]] type.
The [[Niemeier lattice]] with root system <math>D_{24}</math> can be made into a module
for the ring of integers of the field <math>\mathbb{Q}(\sqrt{-23})</math>. Multiplying this
Niemeier lattice by a non-principal ideal of the ring of integers gives the Leech lattice.

===Using higher power residue codes===
{{harvtxt|Raji|2005}} constructed the Leech lattice using higher power residue codes over the ring <math>Z_4</math>. A similar construction is used to construct some of the other lattices of rank 24.

===Using octonions===
If ''L'' is the set of [[octonion]]s with coordinates on the <math>E_8</math> [[E8_lattice|lattice]], then the Leech lattice is the set of triplets <math>(x,y,z)</math> such that

:<math>x,y,z \in L</math>

:<math>x+y+z \in Ls</math>

:<math>x+y,\ y+z,\ x+z \in L\bar{s}</math>

where <math>s= \frac 1 2 (-e_1 + e_2 + e_3 + e_4 + e_5 + e_6 + e_7)</math>.  This construction is due to {{harv|Wilson|2009}}.

==Symmetries==

The Leech lattice is highly symmetrical.  Its [[automorphism group]] is the [[Conway group]] Co<sub>0</sub>, which is of order  8&nbsp;315&nbsp;553&nbsp;613&nbsp;086&nbsp;720&nbsp;000.  The center of Co<sub>0</sub> has two elements, and the quotient of Co<sub>0</sub> by this center is the Conway group Co<sub>1</sub>, a finite simple group.  Many other [[sporadic group]]s, such as the remaining Conway groups and [[Mathieu groups]], can be constructed as the stabilizers of various configurations of vectors in the Leech lattice.

Despite having such a high ''rotational'' symmetry group, the Leech lattice does not possess any hyperplanes of reflection symmetry. In other words, the Leech lattice is [[chiral]]. It also has far fewer symmetries than the 24-dimensional hypercube and simplex, or even the Cartesian product of three copies of the [[E8 lattice]].

The automorphism group was first described by [[John Horton Conway|John Conway]]. The 398034000 vectors of norm 8 fall into 8292375 'crosses' of 48 vectors. Each cross contains 24 mutually orthogonal vectors and their negatives, and thus describe the vertices of a 24-dimensional [[orthoplex]]. Each of these crosses can be taken to be the coordinate system of the lattice, and has the same symmetry of the [[Binary Golay code|Golay code]], namely 2<sup>12</sup> &times; |M<sub>24</sub>|. Hence the full automorphism group of the Leech lattice has order 8292375 &times; 4096 &times; 244823040, or 8&nbsp;315&nbsp;553&nbsp;613&nbsp;086&nbsp;720&nbsp;000.

==Geometry==

{{harvtxt|Conway|Parker|Sloane|1982}} showed that the covering radius of the Leech lattice is <math>\sqrt 2</math>; in other words, if we put a closed ball of this radius around each lattice point, then these just cover Euclidean space. The points at distance at least <math>\sqrt 2</math> from all lattice points are called the '''''deep holes''''' of the Leech lattice. There are 23 orbits of them under the automorphism group of the Leech lattice, and these orbits correspond to the 23 [[Niemeier lattices]] other than the Leech lattice: the set of vertices of  deep hole is isometric to the affine Dynkin diagram of the corresponding Niemeier lattice.

The Leech lattice has a density of <math>\tfrac{\pi^{12}}{12!}\approx 0.001930</math>. {{harvtxt|Cohn|Kumar|2009}} showed that it gives the densest lattice [[sphere packing|packing of balls]] in 24-dimensional space. {{harvs|txt|title=The sphere packing problem in dimension 24|
first1=Henry|last1= Cohn|first2= Abhinav|last2= Kumar|first3= Stephen D. |last3=Miller|first4= Danylo |last4=Radchenko|first5= Maryna |last5=Viazovska|year=2017|arxiv=1603.06518}} improved this by showing that it is the densest sphere packing, even among non-lattice packings.

The 196560 minimal vectors are of three different varieties, known as ''shapes'':

* <math>1104 = \binom {24}{2} \cdot 2^2</math> vectors of shape (4<sup>2</sup>,0<sup>22</sup>), for all permutations and sign choices;
* <math>97152 = 759 \cdot 2^8 \cdot \frac {1}{2}</math> vectors of shape (2<sup>8</sup>,0<sup>16</sup>), where the '2's correspond to an octad in the Golay code, and there are any even number of minus signs;
* <math>98304 = 2^{12} \cdot 24</math> vectors of shape (∓3,±1<sup>23</sup>), where the lower sign is used for the '1's of any codeword of the Golay code, and the '∓3' can appear in any position.

The [[ternary Golay code]], [[binary Golay code]] and Leech lattice give very efficient 24-dimensional [[spherical code]]s of 729, 4096 and 196560 points, respectively. Spherical codes are higher-dimensional analogues of [[Tammes problem]], which arose as an attempt to explain the distribution of pores on pollen grains. These are distributed as to maximise the minimal angle between them. In two dimensions, the problem is trivial, but in three dimensions and higher it is not. An example of a spherical code in three dimensions is the set of the 12 vertices of the regular icosahedron.

==Theta series==

One can associate to any (positive-definite) lattice Λ a [[theta function]] given by

:<math>\Theta_\Lambda(\tau) = \sum_{x\in\Lambda} e^{i\pi\tau\|x\|^2} \qquad \operatorname{Im} \tau > 0.</math>

The theta function of a lattice is then a [[holomorphic function]] on the [[upper half-plane]]. Furthermore, the theta function of an even unimodular lattice of rank ''n'' is actually a [[modular form]] of weight ''n''/2 for the full [[modular group]] PSL(2,'''Z'''). The theta function of an integral lattice is often written as a [[power series]] in <math>q = e^{2i\pi\tau}</math> so that the coefficient of ''q''<sup>''n''</sup> gives the number of lattice vectors of squared norm 2''n''. In the Leech lattice, there are 196560 vectors of squared norm 4, 16773120 vectors of squared norm 6, 398034000 vectors of squared norm 8 and so on. The theta series of the Leech lattice is

: <math>
\begin{align}
\Theta_{\Lambda_{24}}(\tau) & = E_{12}(\tau)-\frac{65520}{691} \Delta(\tau) \\[5pt]
& = 1 + \sum_{m=1}^\infty \frac{65520}{691} \left(\sigma_{11} (m) - \tau (m) \right) q^m \\[5pt]
& = 1 + 196560q^2 + 16773120q^3 + 398034000q^4 + \cdots,
\end{align}
</math>

where <math>E_{12}(\tau)</math> is the normalized [[Eisenstein series]] of weight 12, <math>\Delta(\tau)</math> is the [[modular discriminant]], <math>\sigma_{11}(n)</math> is the [[divisor function]] for exponent 11, and <math>\tau(n)</math> is the [[Ramanujan tau function]]. It follows that for ''m''≥1 the number of vectors of squared norm 2''m'' is

: <math> \frac{65520}{691} \left(\sigma_{11} (m) - \tau (m) \right).</math>

==History==
Many of the cross-sections of the Leech lattice, including the [[Coxeter&ndash;Todd lattice]] and [[Barnes&ndash;Wall lattice]], in 12 and 16 dimensions, were found much earlier than the Leech lattice. {{harvtxt|O'Connor|Pall|1944}} discovered a related odd unimodular lattice in 24 dimensions, now called the ''odd Leech lattice'', one of whose two even neighbors is the Leech lattice. The  Leech lattice was discovered in 1965 by {{harvs|txt|authorlink=John Leech (mathematician)|first=John|last= Leech|year=1967|loc=2.31, p. 262}}, by improving some earlier sphere packings he found {{harv|Leech|1964}}.

{{harvs|txt|authorlink=John Horton Conway|last=Conway|year=1968}} calculated the order of the [[automorphism group]] of the Leech lattice, and, working with [[John G. Thompson]], discovered three new [[sporadic group]]s as a by-product: the [[Conway groups]], Co<sub>1</sub>, Co<sub>2</sub>, Co<sub>3</sub>. They also showed that four other (then) recently announced sporadic groups, namely, [[Higman-Sims group|Higman-Sims]], [[Suzuki sporadic group|Suzuki]], [[McLaughlin group (mathematics)|McLaughlin]], and the [[Janko group]] J<sub>2</sub> could be found inside the Conway groups using the geometry of the Leech lattice. (Ronan, p.&nbsp;155)

{{quote box
|align=right
|width=33%
|quote=Bei dem Versuch, eine Form aus einer solchen Klasse wirklich anzugeben, fand ich mehr als 10 verschiedene Klassen in Γ<sub>24</sub>
|source={{harvtxt|Witt|1941|loc=p. 324}}
}}
{{harvtxt|Witt|1941|loc=p. 324}},  has a single rather cryptic sentence mentioning that he found  more than 10 even unimodular lattices in 24 dimensions without giving further details. {{harvtxt|Witt|1998|loc=p. 328–329}} stated that he found 9 of these lattices earlier in 1938, and found two more, the [[Niemeier lattice]] with A{{su|p=24|b=1}} root system and the Leech lattice (and also the odd Leech lattice), in 1940.

==See also==
*[[Sphere packing]]
*[[E8 lattice|E<sub>8</sub> lattice]]

==References==
{{Reflist}}

*{{Citation |  last1=Chapman | first1=Robin | title=Conference matrices and unimodular lattices | doi=10.1006/eujc.2001.0539 | mr=1861046  | zbl=0993.05036 | year=2001 | journal=European Journal of Combinatorics | issn=0195-6698 | volume=22 | issue=8 | pages=1033–1045 | arxiv=math.NT/0007116 | s2cid=744078 }}
*{{Citation |  last1=Raji | first1=Mehrdad Ahmadzadeh | title=Higher Power Residue Codes and the Leech Lattice | doi=10.1007/s10801-005-6279-4 | year=2005 | journal=Journal of Algebraic Combinatorics | issn=1572-9192 | volume=21 | issue=1 | pages=39–53  | s2cid=120908420 | doi-access=free }}
*{{Citation |  last1=Cohn | first1=Henry | last2=Kumar | first2=Abhinav | title=Optimality and uniqueness of the Leech lattice among lattices | doi=10.4007/annals.2009.170.1003 | mr=2600869 | zbl=1213.11144 | year=2009 | journal=Annals of Mathematics | issn=1939-8980 | volume=170 | issue=3 | pages=1003–1050 | arxiv=math.MG/0403263 | s2cid=10696627 }}
*{{Citation | last1=Cohn | first1=Henry | last2=Kumar | first2=Abhinav | title=The densest lattice in twenty-four dimensions | doi=10.1090/S1079-6762-04-00130-1  | mr=2075897  | year=2004 | journal=Electronic Research Announcements of the American Mathematical Society | issn=1079-6762 | volume=10 | issue=7 | pages=58–67  |arxiv=math.MG/0408174 | bibcode=2004math......8174C | s2cid=15874595 }}
*{{citation|title=The sphere packing problem in dimension 24|
journal=Annals of Mathematics|
volume=185|
issue=3|
pages=1017–1033|
first1=Henry|last1= Cohn|first2= Abhinav|last2= Kumar|first3= Stephen D. |last3=Miller|first4= Danylo |last4=Radchenko|first5= Maryna |last5=Viazovska|authorlink5=Maryna Viazovska|year=2017|arxiv=1603.06518|bibcode=2016arXiv160306518C|
doi=10.4007/annals.2017.185.3.8|
s2cid=119281758}}
*{{Citation | last1=Conway | first1=John Horton | author1-link=John Horton Conway | title=A perfect group of order 8,315,553,613,086,720,000 and the sporadic simple groups | mr=0237634 | year=1968 | journal=[[Proceedings of the National Academy of Sciences|Proceedings of the National Academy of Sciences of the United States of America]] | volume=61 | pages=398–400 | doi=10.1073/pnas.61.2.398 | pmid=16591697 | issue=2| pmc=225171 | bibcode=1968PNAS...61..398C | doi-access=free }}
*{{Citation | last1=Conway | first1=John Horton | author1-link=John Horton Conway | title=The automorphism group of the 26-dimensional even unimodular Lorentzian lattice | doi=10.1016/0021-8693(83)90025-X | mr=690711 | year=1983 | journal=[[Journal of Algebra]] | issn=0021-8693 | volume=80 | issue=1 | pages=159–163| doi-access=free }}
*{{Citation | last1=Conway | first1=John Horton | author1-link=John Horton Conway | last2=Sloane | first2=N. J. A. | author2-link=Neil Sloane | title=Laminated lattices | doi=10.2307/2007025 | mr=678483 | year=1982b | journal=[[Annals of Mathematics]] |series=Second Series | issn=0003-486X | volume=116 | issue=3 | pages=593–620| jstor=2007025 }}
*{{Citation | last1=Conway | first1=John Horton | author1-link=John Horton Conway | last2=Parker | first2=R. A. | last3=Sloane | first3=N. J. A. | author3-link=Neil Sloane | title=The covering radius of the Leech lattice | doi=10.1098/rspa.1982.0042 | mr=660415 | year=1982 | journal=[[Proceedings of the Royal Society A]] | issn=0080-4630 | volume=380 | issue=1779 | pages=261–290| bibcode=1982RSPSA.380..261C | s2cid=202575323 }}
*{{Citation | last1=Conway | first1=John Horton | author1-link=John Horton Conway | last2=Sloane | first2=N. J. A. | author2-link=Neil Sloane | title=Twenty-three constructions for the Leech lattice | doi=10.1098/rspa.1982.0071 | mr=661720 | year=1982 | journal=[[Proceedings of the Royal Society A]] | issn=0080-4630 | volume=381 | issue=1781 | pages=275–283| bibcode=1982RSPSA.381..275C | s2cid=202575295 }}
*{{citation | zbl=0915.52003 | last1=Conway | first1=J.H. | author1-link=John Horton Conway | last2=Sloane | first2=N.J.A. | author2-link=Neil Sloane | others=With contributions by Bannai, E.; Borcherds, R. E.; Leech, J.; Norton, S. P.; Odlyzko, A. M.; Parker, R.A.; Queen, L.; Venkov, B.B. | title=Sphere packings, lattices and groups | edition=Third | series=Grundlehren der Mathematischen Wissenschaften | volume=290 | location=New York, NY | publisher=[[Springer-Verlag]] | isbn=978-0-387-98585-5 | mr=662447 | year=1999 | url-access=registration | url=https://archive.org/details/spherepackingsla0000conw_b8u0 }}
*{{citation | first=Marcus| last=Du Sautoy | title=Finding Moonshine | isbn=978-0-00-721462-4 | publisher=Fourth Estate| year=2009 }}
*{{citation | last=Griess | first=Robert L. | title=Twelve Sporadic Groups | publisher=Springer-Verlag | year=1998 | series=Springer Monographs in Mathematics | location=Berlin | isbn=978-3-540-62778-4 | doi=10.1007/978-3-662-03516-0 | mr=1707296}}
*{{Citation | last1=Leech | first1=John | title=Some sphere packings in higher space | doi=10.4153/CJM-1964-065-1 | mr=0167901 | year=1964 | journal=[[Canadian Journal of Mathematics]] | issn=0008-414X | volume=16 | pages=657–682| s2cid=123244939 | doi-access=free }}
*{{Citation | last1=Leech | first1=John | title=Notes on sphere packings | doi=10.4153/CJM-1967-017-0 | mr=0209983 | year=1967 | journal=[[Canadian Journal of Mathematics]] | issn=0008-414X | volume=19 | pages=251–267| doi-access=free }}
*{{Citation | last1=O'Connor | first1=R. E. | last2=Pall | first2=G. | title=The construction of integral quadratic forms of determinant 1 | doi=10.1215/S0012-7094-44-01127-0 | mr=0010153 | year=1944 | journal=[[Duke Mathematical Journal]] | issn=0012-7094 | volume=11 | issue=2 | pages=319–331}}
*{{citation | last=Thompson | first=Thomas M | title=From Error Correcting Codes through Sphere Packings to Simple Groups | series=Carus Mathematical Monographs | publisher=Mathematical Association of America | year=1983 | mr=0749038 | volume=21 | location=Washington, DC | isbn=978-0-88385-023-7}}
*{{citation | last=Ronan | first=Mark | title=Symmetry and the Monster | publisher=Oxford University Press| isbn=978-0-19-280722-9 | location=Oxford | year=2006 | mr=2215662}}
*{{Citation | last1=Wilson | first1=Robert A. | title=Octonions and the Leech lattice | mr=2542837 | year=2009 | journal=Journal of Algebra | volume=322 | issue=6 | pages=2186–2190| doi=10.1016/j.jalgebra.2009.03.021 | doi-access=free }}
*{{Citation | last1=Witt | first1=Ernst | author1-link=Ernst Witt | title=Eine Identität zwischen Modulformen zweiten Grades | doi=10.1007/BF02940750 | mr=0005508 | year=1941 | journal=Abhandlungen aus dem Mathematischen Seminar der Universität Hamburg | volume=14 | pages=323–337| s2cid=120849019 }}
*{{Citation | last1=Witt | first1=Ernst | author1-link=Ernst Witt | title=Collected papers. Gesammelte Abhandlungen | publisher=[[Springer-Verlag]] | location=Berlin, New York | isbn=978-3-540-57061-5 | mr=1643949 | year=1998}}

==External links==
*[http://cp4space.wordpress.com/2013/09/12/leech-lattice/ Leech lattice (CP4space)]
*{{MathWorld|id=LeechLattice}}
*[https://web.archive.org/web/20110727121450/http://www.math.uic.edu/~ronan/Leech_Lattice The Leech Lattice, U. of Illinois at Chicago, Mark Ronan's website]
*[http://math.berkeley.edu/~reb/papers/ Papers by R. E. Borcherds]

{{DEFAULTSORT:Leech Lattice}}
[[Category:Quadratic forms]]
[[Category:Lattice points]]
[[Category:Sporadic groups]]
[[Category:Moonshine theory]]