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Algebraic structures between magmas and groups: A quasigroup is a magma with the type of divisibility given by the Latin square property. A loop is a quasigroup with an identity element.

In mathematics, especially in abstract algebra, a quasigroup is an algebraic structure that resembles a group in the sense that "division" is always possible. Quasigroups differ from groups mainly in that the associative and identity element properties are optional. In fact, a nonempty associative quasigroup is a group.[1][2]

A quasigroup that has an identity element is called a loop[3].

Definitions

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There are at least two structurally equivalent formal definitions of a quasigroup:

The homomorphic image of a quasigroup that is defined with a single binary operation, however, need not be a quasigroup, in contrast to a quasigroup as having three primitive operations.[4] We begin with the first definition.

Algebra

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A quasigroup (Q, ∗) is a set Q with a binary operation (that is, a magma, indicating that a quasigroup has to satisfy the closure property), obeying the Latin square property. This states that, for each a and b in Q, there exist unique elements x and y in Q such that both hold. (In other words: Each element of the set occurs exactly once in each row and exactly once in each column of the quasigroup's multiplication table, or Cayley table. This property ensures that the Cayley table of a finite quasigroup, and, in particular, a finite group, is a Latin square.) The requirement that x and y be unique can be replaced by the requirement that the magma be cancellative.[5][a]

The unique solutions to these equations are written x = a \ b and y = b / a. The operations '\' and '/' are called, respectively, left division and right division. With regard to the Cayley table, the first equation (left division) means that the b entry in the a row is in the x column while the second equation (right division) means that the b entry in the a column is in the y row.

The empty set equipped with the empty binary operation satisfies this definition of a quasigroup. Some authors accept the empty quasigroup, but others explicitly exclude it.[6][7]

Universal algebra

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Given some algebraic structure, an identity is an equation in which all variables are tacitly universally quantified, and in which all operations are among the primitive operations proper to the structure. Algebraic structures that satisfy axioms that are given solely by identities are called varieties. Many standard results in universal algebra hold only for varieties. Quasigroups form a variety if left and right division are taken as primitive.

A right-quasigroup (Q, ∗, /) is a type (2, 2) algebra that satisfies the identities:

A left-quasigroup (Q, ∗, \) is a type (2, 2) algebra that satisfies the identities:

A quasigroup (Q, ∗, \, /) is a type (2, 2, 2) algebra (i.e., equipped with three binary operations) that satisfies the identities:[b]

In other words: Multiplication and division in either order, one after the other, on the same side by the same element, have no net effect.

Hence if (Q, ∗) is a quasigroup according to the definition of the previous section, then (Q, ∗, \, /) is the same quasigroup in the sense of universal algebra. And vice versa: if (Q, ∗, \, /) is a quasigroup according to the sense of universal algebra, then (Q, ∗) is a quasigroup according to the first definition.

Loops

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A loop is a quasigroup with an identity element; that is, an element, e, such that

xe = x and ex = x for all x in Q.

It follows that the identity element, e, is unique, and that every element of Q has unique left and right inverses (which need not be the same). Since the presence of an identity element is essential, a loop cannot be empty.

A quasigroup with an idempotent element is called a pique ("pointed idempotent quasigroup"); this is a weaker notion than a loop but common nonetheless because, for example, given an abelian group, (A, +), taking its subtraction operation as quasigroup multiplication yields a pique (A, −) with the group identity (zero) turned into a "pointed idempotent". (That is, there is a principal isotopy (x, y, z) ↦ (x, −y, z).)

A loop that is associative is a group. A group can have a strictly nonassociative pique isotope, but it cannot have a strictly nonassociative loop isotope.

There are weaker associativity properties that have been given special names.

For instance, a Bol loop is a loop that satisfies either:

x ∗ (y ∗ (xz)) = (x ∗ (yx)) ∗ z     for each x, y and z in Q (a left Bol loop),

or else

((zx) ∗ y) ∗ x = z ∗ ((xy) ∗ x)     for each x, y and z in Q (a right Bol loop).

A loop that is both a left and right Bol loop is a Moufang loop. This is equivalent to any one of the following single Moufang identities holding for all x, y, z:

x ∗ (y ∗ (xz)) = ((xy) ∗ x) ∗ z
z ∗ (x ∗ (yx)) = ((zx) ∗ y) ∗ x
(xy) ∗ (zx) = x ∗ ((yz) ∗ x)
(xy) ∗ (zx) = (x ∗ (yz)) ∗ x.

According to Jonathan D. H. Smith, "loops" were named after the Chicago Loop, as their originators were studying quasigroups in Chicago at the time.[10]

Symmetries

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Smith (2007) names the following important properties and subclasses:

Semisymmetry

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A quasigroup is semisymmetric if any of the following equivalent identities hold for all x, y:[c]

xy = y / x
yx = x \ y
x = (yx) ∗ y
x = y ∗ (xy).

Although this class may seem special, every quasigroup Q induces a semisymmetric quasigroup QΔ on the direct product cube Q3 via the following operation:

(x1, x2, x3) ⋅ (y1, y2, y3) = (y3 / x2, y1 \ x3, x1y2) = (x2 // y3, x3 \\ y1, x1y2),

where "//" and "\\" are the conjugate division operations given by y // x = x / y and y \\ x = x \ y.

Triality

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A quasigroup may exhibit semisymmetric triality.[11]

Total symmetry

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A narrower class is a totally symmetric quasigroup (sometimes abbreviated TS-quasigroup) in which all conjugates coincide as one operation: xy = x / y = x \ y. Another way to define (the same notion of) totally symmetric quasigroup is as a semisymmetric quasigroup that is commutative, i.e. xy = yx.

Idempotent total symmetric quasigroups are precisely (i.e. in a bijection with) Steiner triples, so such a quasigroup is also called a Steiner quasigroup, and sometimes the latter is even abbreviated as squag. The term sloop refers to an analogue for loops, namely, totally symmetric loops that satisfy xx = 1 instead of xx = x. Without idempotency, total symmetric quasigroups correspond to the geometric notion of extended Steiner triple, also called Generalized Elliptic Cubic Curve (GECC).

Total antisymmetry

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A quasigroup (Q, ∗) is called weakly totally anti-symmetric if for all c, x, yQ, the following implication holds.[12]

(cx) ∗ y = (cy) ∗ x implies that x = y.

A quasigroup (Q, ∗) is called totally anti-symmetric if, in addition, for all x, yQ, the following implication holds:[12]

xy = yx implies that x = y.

This property is required, for example, in the Damm algorithm.

Examples

[edit]
  • Every group is a loop, because ax = b if and only if x = a−1b, and ya = b if and only if y = ba−1.
  • The integers Z (or the rationals Q or the reals R) with subtraction (−) form a quasigroup. These quasigroups are not loops because there is no identity element (0 is a right identity because a − 0 = a, but not a left identity because, in general, 0 − aa).
  • The nonzero rationals Q× (or the nonzero reals R×) with division (÷) form a quasigroup.
  • Any vector space over a field of characteristic not equal to 2 forms an idempotent, commutative quasigroup under the operation xy = (x + y) / 2.
  • Every Steiner triple system defines an idempotent, commutative quasigroup: ab is the third element of the triple containing a and b. These quasigroups also satisfy (xy) ∗ y = x for all x and y in the quasigroup. These quasigroups are known as Steiner quasigroups.[13]
  • The set {±1, ±i, ±j, ±k} where ii = jj = kk = +1 and with all other products as in the quaternion group forms a nonassociative loop of order 8. See hyperbolic quaternions for its application. (The hyperbolic quaternions themselves do not form a loop or quasigroup.)
  • The nonzero octonions form a nonassociative loop under multiplication. The octonions are a special type of loop known as a Moufang loop.
  • An associative quasigroup is either empty or is a group, since if there is at least one element, the invertibility of the quasigroup binary operation combined with associativity implies the existence of an identity element, which then implies the existence of inverse elements, thus satisfying all three requirements of a group.
  • The following construction is due to Hans Zassenhaus. On the underlying set of the four-dimensional vector space F4 over the 3-element Galois field F = Z/3Z define
    (x1, x2, x3, x4) ∗ (y1, y2, y3, y4) = (x1, x2, x3, x4) + (y1, y2, y3, y4) + (0, 0, 0, (x3y3)(x1y2x2y1)).
Then, (F4, ∗) is a commutative Moufang loop that is not a group.[14]
  • More generally, the nonzero elements of any division algebra form a quasigroup with the operation of multiplication in the algebra.

Properties

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In the remainder of the article we shall denote quasigroup multiplication simply by juxtaposition.

Quasigroups have the cancellation property: if ab = ac, then b = c. This follows from the uniqueness of left division of ab or ac by a. Similarly, if ba = ca, then b = c.

The Latin square property of quasigroups implies that, given any two of the three variables in xy = z, the third variable is uniquely determined.

Multiplication operators

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The definition of a quasigroup can be treated as conditions on the left and right multiplication operators Lx, Rx : QQ, defined by

Lx(y) = xy
Rx(y) = yx

The definition says that both mappings are bijections from Q to itself. A magma Q is a quasigroup precisely when all these operators, for every x in Q, are bijective. The inverse mappings are left and right division, that is,

L−1
x
(y) = x \ y
R−1
x
(y) = y / x

In this notation the identities among the quasigroup's multiplication and division operations (stated in the section on universal algebra) are

LxL−1
x
= id            corresponding to            x(x \ y) = y
L−1
x
Lx = id            corresponding to            x \ (xy) = y
RxR−1
x
= id            corresponding to            (y / x)x = y
R−1
x
Rx = id            corresponding to            (yx) / x = y

where id denotes the identity mapping on Q.

Latin squares

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A Latin square, the unbordered multiplication table for a quasigroup whose 10 elements are the digits 0–9.
0 4 8 2 3 9 6 7 1 5
3 6 2 8 7 1 9 5 0 4
8 9 3 1 0 6 4 2 5 7
1 7 6 5 4 8 0 3 2 9
2 1 9 0 6 7 5 8 4 3
5 2 7 4 9 3 1 0 8 6
4 3 0 6 1 5 2 9 7 8
9 8 5 7 2 0 3 4 6 1
7 0 1 9 5 4 8 6 3 2
6 5 4 3 8 2 7 1 9 0

The multiplication table of a finite quasigroup is a Latin square: an n × n table filled with n different symbols in such a way that each symbol occurs exactly once in each row and exactly once in each column.

Conversely, every Latin square can be taken as the multiplication table of a quasigroup in many ways: the border row (containing the column headers) and the border column (containing the row headers) can each be any permutation of the elements. See Small Latin squares and quasigroups.

Infinite quasigroups

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For a countably infinite quasigroup Q, it is possible to imagine an infinite array in which every row and every column corresponds to some element q of Q, and where the element ab is in the row corresponding to a and the column responding to b. In this situation too, the Latin square property says that each row and each column of the infinite array will contain every possible value precisely once.

For an uncountably infinite quasigroup, such as the group of non-zero real numbers under multiplication, the Latin square property still holds, although the name is somewhat unsatisfactory, as it is not possible to produce the array of combinations to which the above idea of an infinite array extends since the real numbers cannot all be written in a sequence. (This is somewhat misleading however, as the reals can be written in a sequence of length , assuming the well-ordering theorem.)

Inverse properties

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The binary operation of a quasigroup is invertible in the sense that both Lx and Rx, the left and right multiplication operators, are bijective, and hence invertible.

Every loop element has a unique left and right inverse given by

xλ = e / x            xλx = e
xρ = x \ e            xxρ = e

A loop is said to have (two-sided) inverses if xλ = xρ for all x. In this case the inverse element is usually denoted by x−1.

There are some stronger notions of inverses in loops that are often useful:

  • A loop has the left inverse property if xλ(xy) = y for all x and y. Equivalently, L−1
    x
    = Lxλ
    or x \ y = xλy.
  • A loop has the right inverse property if (yx)xρ = y for all x and y. Equivalently, R−1
    x
    = Rxρ
    or y / x = yxρ.
  • A loop has the antiautomorphic inverse property if (xy)λ = yλxλ or, equivalently, if (xy)ρ = yρxρ.
  • A loop has the weak inverse property when (xy)z = e if and only if x(yz) = e. This may be stated in terms of inverses via (xy)λx = yλ or equivalently x(yx)ρ = yρ.

A loop has the inverse property if it has both the left and right inverse properties. Inverse property loops also have the antiautomorphic and weak inverse properties. In fact, any loop that satisfies any two of the above four identities has the inverse property and therefore satisfies all four.

Any loop that satisfies the left, right, or antiautomorphic inverse properties automatically has two-sided inverses.

Morphisms

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A quasigroup or loop homomorphism is a map f : QP between two quasigroups such that f(xy) = f(x)f(y). Quasigroup homomorphisms necessarily preserve left and right division, as well as identity elements (if they exist).

Homotopy and isotopy

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Let Q and P be quasigroups. A quasigroup homotopy from Q to P is a triple (α, β, γ) of maps from Q to P such that

α(x)β(y) = γ(xy)

for all x, y in Q. A quasigroup homomorphism is just a homotopy for which the three maps are equal.

An isotopy is a homotopy for which each of the three maps (α, β, γ) is a bijection. Two quasigroups are isotopic if there is an isotopy between them. In terms of Latin squares, an isotopy (α, β, γ) is given by a permutation of rows α, a permutation of columns β, and a permutation on the underlying element set γ.

An autotopy is an isotopy from a quasigroup to itself. The set of all autotopies of a quasigroup forms a group with the automorphism group as a subgroup.

Every quasigroup is isotopic to a loop. If a loop is isotopic to a group, then it is isomorphic to that group and thus is itself a group. However, a quasigroup that is isotopic to a group need not be a group. For example, the quasigroup on R with multiplication given by (x, y) ↦ (x + y)/2 is isotopic to the additive group (R, +), but is not itself a group as it has no identity element. Every medial quasigroup is isotopic to an abelian group by the Bruck–Toyoda theorem.

Conjugation (parastrophe)

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Left and right division are examples of forming a quasigroup by permuting the variables in the defining equation. From the original operation ∗ (i.e., xy = z) we can form five new operations: x o y := yx (the opposite operation), / and \, and their opposites. That makes a total of six quasigroup operations, which are called the conjugates or parastrophes of ∗. Any two of these operations are said to be "conjugate" or "parastrophic" to each other (and to themselves).

Isostrophe (paratopy)

[edit]

If the set Q has two quasigroup operations, ∗ and ·, and one of them is isotopic to a conjugate of the other, the operations are said to be isostrophic to each other. There are also many other names for this relation of "isostrophe", e.g., paratopy.

Generalizations

[edit]

Polyadic or multiary quasigroups

[edit]

An n-ary quasigroup is a set with an n-ary operation, (Q, f) with f : QnQ, such that the equation f(x1, ..., xn) = y has a unique solution for any one variable if all the other n variables are specified arbitrarily. Polyadic or multiary means n-ary for some nonnegative integer n.

A 0-ary, or nullary, quasigroup is just a constant element of Q. A 1-ary, or unary, quasigroup is a bijection of Q to itself. A binary, or 2-ary, quasigroup is an ordinary quasigroup.

An example of a multiary quasigroup is an iterated group operation, y = x1 · x2 · ··· · xn; it is not necessary to use parentheses to specify the order of operations because the group is associative. One can also form a multiary quasigroup by carrying out any sequence of the same or different group or quasigroup operations, if the order of operations is specified.

There exist multiary quasigroups that cannot be represented in any of these ways. An n-ary quasigroup is irreducible if its operation cannot be factored into the composition of two operations in the following way:

f(x1, ..., xn) = g(x1, ..., xi−1, h(xi, ..., xj), xj+1, ..., xn),

where 1 ≤ i < jn and (i, j) ≠ (1, n). Finite irreducible n-ary quasigroups exist for all n > 2; see Akivis & Goldberg (2001) for details.

An n-ary quasigroup with an n-ary version of associativity is called an n-ary group.

Number of small quasigroups and loops

[edit]

The number of isomorphism classes of small quasigroups (sequence A057991 in the OEIS) and loops (sequence A057771 in the OEIS) is given here:[15]

Order Number of quasigroups Number of loops
0 1 0
1 1 1
2 1 1
3 5 1
4 35 2
5 1411 6
6 1130531 109
7 12198455835 23746
8 2697818331680661 106228849
9 15224734061438247321497 9365022303540
10 2750892211809150446995735533513 20890436195945769617
11 19464657391668924966791023043937578299025 1478157455158044452849321016

See also

[edit]

Notes

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References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
In mathematics, a quasigroup is a set QQ equipped with a binary operation \cdot such that, for all a,bQa, b \in Q, the equations ax=ba \cdot x = b and ya=by \cdot a = b have unique solutions x,yQx, y \in Q. This property ensures that left and right multiplications by any element are bijective permutations of QQ, and the multiplication table of a finite quasigroup corresponds to a Latin square, where each symbol appears exactly once in every row and column. Equivalently, a quasigroup can be defined using three binary operations—multiplication \cdot, left division \\backslash, and right division //—satisfying identities such as x(x\y)=yx \cdot (x \backslash y) = y and (y/x)x=y(y / x) \cdot x = y. Quasigroups generalize groups by relaxing the requirements of associativity and identity elements, forming a foundational structure in non-associative algebra that emerged in the late 19th century as part of early studies in algebra and combinatorics, with the term "quasigroup" coined by Ruth Moufang in 1935 during her work on non-Desarguesian projective planes. Key developments in the 1930s and 1940s, including contributions from mathematicians like A. A. Sushkevich, Ruth Moufang, and R. H. Bruck, established connections to loops (quasigroups with an identity element) and medial quasigroups (those satisfying (xy)(uv)=(xu)(yv)(xy)(uv) = (xu)(yv)), which are affine over abelian groups via the Toyoda-Murdoch-Bruck theorem. Notable subclasses include Moufang quasigroups, which satisfy identities like x(y(xz))=((xy)z)xx(y(xz)) = ((xy)z)x, and quandles, idempotent right-distributive quasigroups used in knot theory. Examples of quasigroups abound: any group is an associative quasigroup, the integers under form a quasigroup without identity, and the operation on a defined by a yields a quasigroup of that order. The number of quasigroups of order nn grows rapidly—12 for n=3n=3, 576 for n=4n=4—and every quasigroup is isotopic to at least one loop, meaning there exist bijections aligning the operations up to of variables. Quasigroups find applications across mathematics, including the construction of Steiner triple systems and projective planes via coordinatization, cryptography through quasigroup string transformations and stream ciphers, and knot invariants via associated quandles, as developed by David Joyce in 1982. Their multiplication groups, permutations generated by left and right translations, provide a group-theoretic lens for studying structure and symmetry.

Definitions

Algebraic Definition

A quasigroup is an consisting of a set QQ together with a :Q×QQ\cdot: Q \times Q \to Q such that, for all a,bQa, b \in Q, the equations ax=ba \cdot x = b and ya=by \cdot a = b possess unique solutions x,yQx, y \in Q. This divisibility condition implies that the left La:QQL_a: Q \to Q defined by La(x)=axL_a(x) = a \cdot x and the right Ra:QQR_a: Q \to Q defined by Ra(x)=xaR_a(x) = x \cdot a are bijective for every aQa \in Q. The unique solvability enables the definition of division operations within the quasigroup. The right division a/ba / b is the unique element xQx \in Q satisfying ax=ba \cdot x = b, while the left division b\ab \backslash a is the unique element yQy \in Q satisfying ya=by \cdot a = b. These operations extend the binary into a partial with inverses in a generalized sense, distinguishing quasigroups from more restrictive s like groups, which additionally require associativity and an . For a finite quasigroup of order nn, the multiplication table—where rows and columns are indexed by elements of QQ and entries are given by the operation—forms a of order nn. In this square, each symbol from QQ appears exactly once in every row and every column, reflecting the bijectivity of the multiplication maps. This connection underscores the combinatorial significance of quasigroups. The concept of quasigroups emerged in the 1930s, with the term "quasigroup" coined by Ruth Moufang in her investigations of non-Desarguesian projective planes, where such structures arose naturally. This development built upon Leonhard Euler's foundational 18th-century work on , including his studies of orthogonal arrays and the 36 officers problem. A simple infinite example is the set of integers Z\mathbb{Z} under subtraction, denoted (Z,)(\mathbb{Z}, -), where ab=aba \cdot b = a - b. For any a,b,cZa, b, c \in \mathbb{Z}, the equation ax=ba - x = b solves uniquely to x=abx = a - b, and ya=by - a = b solves to y=a+by = a + b, satisfying the quasigroup axioms. Loops, which are quasigroups equipped with a two-sided identity element, provide a natural extension of this structure.

Universal Algebra Definition

In universal algebra, a quasigroup is defined as the algebra (Q,,/,\)(Q, \cdot, /, \backslash) consisting of a set QQ equipped with three binary operations: multiplication \cdot, right division //, and left division \\backslash, satisfying the identities y=x(x/y),y=x/(xy),y=(y\x)x,y=(yx)\xy = x \cdot (x / y), \quad y = x / (x \cdot y), \quad y = (y \backslash x) \cdot x, \quad y = (y \cdot x) \backslash x for all x,yQx, y \in Q. These identities ensure that the equations ay=ba \cdot y = b and xa=bx \cdot a = b are uniquely solvable for yy and xx, respectively, with the divisions providing the unique solutions. This equational definition with three primitive operations is equivalent to the combinatorial definition using a single where left and right translations are bijective permutations of QQ. Specifically, given a binary quasigroup (Q,)(Q, \cdot), the division operations are uniquely determined by setting b\ab \backslash a as the unique yy such that ya=by \cdot a = b and a/ba / b as the unique xx such that ax=ba \cdot x = b; conversely, the multiplication operation is uniquely determined by the division operations satisfying the defining identities. The class of all quasigroups forms a variety in the sense of universal algebra, meaning it is defined by identities and thus closed under the formation of subalgebras, homomorphic images, and arbitrary direct products. A derived ternary operation on a quasigroup can be introduced as [x,y,z]=(x\y)z=x(y/z)[x, y, z] = (x \backslash y) \cdot z = x \cdot (y / z), where the equality holds by a derived identity of quasigroups ensuring consistency between left and right solvability; this ternary operation satisfies the projection identities [x,y,y]=x[x, y, y] = x and [x,x,z]=z[x, x, z] = z, and more generally the five-variable identities [[x,y,z],u,v]=[[x,u,v],y,z]=[x,[y,z,u],v]=[x,y,[u,v,z]][[x,y,z],u,v] = [[x,u,v],y,z] = [x,[y,z,u],v] = [x,y,[u,v,z]]. The left and right multiplications are defined as the maps La:QQL_a: Q \to Q given by La(x)=axL_a(x) = a \cdot x and Ra:QQR_a: Q \to Q given by Ra(x)=xaR_a(x) = x \cdot a for each aQa \in Q; the defining identities imply that each LaL_a and RaR_a is a bijection (permutation) on QQ.

Basic Structures

Loops

A loop is a quasigroup (Q,)(Q, \cdot) equipped with a two-sided identity element eQe \in Q satisfying ex=xe=xe \cdot x = x \cdot e = x for all xQx \in Q. This structure generalizes groups by relaxing the associativity axiom while preserving the ability to perform unique divisions. The term "loop" was coined in the early 1940s by A. A. Albert and his collaborators in Chicago, evoking the city's famous Loop district and rhyming with "group." Every loop is a quasigroup, as the presence of the identity ensures that left and right multiplications remain bijective, allowing unique solutions to equations of the form ax=ba \cdot x = b and ya=by \cdot a = b. However, the converse fails: not every quasigroup is a loop, since some lack an identity element. A standard example is the set of integers Z\mathbb{Z} under subtraction, where ab=aba * b = a - b; this operation yields a quasigroup, as divisions are uniquely solvable (e.g., solving ax=ba - x = b gives x=abx = a - b), but no element ee satisfies ex=xe - x = x for all xZx \in \mathbb{Z}. In a loop, each element x[Q](/page/Q)x \in [Q](/page/Q) admits a unique left inverse xlx^l such that xlx=ex^l \cdot x = e and a unique right inverse xrx^r such that xxr=ex \cdot x^r = e, with xlx^l and xrx^r not necessarily equal in non-associative cases. These inverses follow directly from the quasigroup divisions: xl=x\ex^l = x \backslash e and xr=e/xx^r = e / x. Groups provide the associative case of loops, where left and right inverses coincide and the operation satisfies (xy)z=x(yz)(xy)z = x(yz) for all x,y,z[Q](/page/Q)x, y, z \in [Q](/page/Q). A prominent non-associative example arises from the of nonzero octonions, which forms a loop (specifically, a Moufang loop) on the 8-dimensional real vector space excluding zero.

Latin Squares

A quasigroup on a of order nn is in one-to-one correspondence with an n×nn \times n , where the of the quasigroup—listing the products aba \cdot b for elements a,ba, b in the set—serves as the Latin square, with rows and columns indexed by the elements and entries being the s from the set. This arises because the quasigroup axioms ensure that left and right multiplications are bijective, guaranteeing that each symbol appears exactly once in every row and column of the table. Conversely, any Latin square defines a quasigroup operation via its table, as the unique entry in each position satisfies the solvability conditions for the quasigroup equations. If the is reduced—meaning its first row and first column are in natural order (1 to nn)—then the corresponding quasigroup is a loop, possessing a two-sided . More generally, two quasigroups are isotopic if there exist bijections α,β,γ\alpha, \beta, \gamma on the underlying set such that α(x)y=γ(xβ(y))\alpha(x) \cdot' y = \gamma(x \cdot \beta(y)) for all x,yx, y, and this relation corresponds precisely to the isotopism of their associated Latin squares, where an isotopism is a triple of permutations on rows, columns, and symbols that transforms one square into the other. Isotopic quasigroups thus share structural similarities, such as having isomorphic multiplication groups, though they may differ in properties like the presence of an identity. Latin squares associated with quasigroups can be constructed using orthogonal mates: if a Latin square LL has an orthogonal mate MM—another Latin square such that the pairs (L(i,j),M(i,j))(L(i,j), M(i,j)) are all distinct—then combining them yields a set of , each corresponding to a quasigroup operation that can be composed to form more complex structures. A prominent construction yields Steiner quasigroups from finite s: given a projective plane of order nn (with n2+n+1n^2 + n + 1 points), the points form the underlying set of a Steiner quasigroup satisfying the identities xx=xx \cdot x = x, xy=yxx \cdot y = y \cdot x, and x(xy)=yx \cdot (x \cdot y) = y, where the operation is defined geometrically using lines of the plane, and its is a symmetric idempotent Latin square. Such quasigroups exist whenever a projective plane of order nn does, which occurs for all nn. The extends to infinite quasigroups: for any set QQ, a quasigroup operation on QQ yields a (possibly infinite) indexed by QQ, where each row and column is a from QQ to itself, ensuring unique solvability of the quasigroup equations. In the countable infinite case, this corresponds to a countable , as seen in constructions over infinite sets like or integers under suitable operations, maintaining the bijective properties without finiteness restrictions.

Examples

Finite Quasigroups

The quasigroup of order 1 consists of a single element ee with the operation defined by ee=ee \cdot e = e. This is a loop, serving as the trivial example where the unique element acts as the identity. For order 2, there is a unique quasigroup up to , given by the set {e,a}\{e, a\} with the : eaeeaaae\begin{array}{c|cc} \cdot & e & a \\ \hline e & e & a \\ a & a & e \\ \end{array} This quasigroup is a loop with identity ee, isomorphic to the Z2\mathbb{Z}_2. Of order 3, there exist five non-isomorphic quasigroups, only one of which is a loop: the Z3\mathbb{Z}_3 under addition, with elements {0,1,2}\{0, 1, 2\} and operation modulo 3. The remaining four are non-loops, illustrating early examples where the representation yields distinct algebraic structures without an . Quasigroups also arise from s through planar functions, which generate commutative quasigroups on the field elements and coordinatize affine planes. For a Fq\mathbb{F}_q and a planar function f:FqFqf: \mathbb{F}_q \to \mathbb{F}_q, the operation xy=f(xy)+yx * y = f(x - y) + y defines a commutative quasigroup whose properties reflect the geometric structure of the associated affine plane of order qq. These quasigroups are quasifields when equipped with additional division properties, enabling the construction of non-Desarguesian affine planes. Steiner triple systems provide another construction of idempotent quasigroups. Given a Steiner triple system STS(vv) on a set of v1v \equiv 1 or 3(mod6)3 \pmod{6} points, define the operation by xx=xx * x = x for all xx, and for xyx \neq y, xy=zx * y = z where {x,y,z}\{x, y, z\} is the unique triple containing xx and yy. The resulting quasigroup is idempotent, commutative, and totally symmetric, with the property that xy=yxx * y = y * x and x(xy)=yx * (x * y) = y. This correspondence links combinatorial designs directly to algebraic structures, as seen in the Fano plane yielding an STS(7) and its associated quasigroup.

Infinite Quasigroups

Infinite quasigroups arise in various algebraic contexts, providing structures on infinite sets where the operation ensures unique solvability of equations without requiring associativity or an identity element. A prominent example is the set of integers Z\mathbb{Z} equipped with the subtraction operation, defined by xy=xyx \cdot y = x - y. This forms a quasigroup because, for any fixed a,bZa, b \in \mathbb{Z}, the equations ax=ba - x = b (solving for x=abx = a - b) and ya=by - a = b (solving for y=a+by = a + b) have unique solutions, and similarly for other combinations. However, it is not a loop, as there is no identity element satisfying xe=xx - e = x and ex=xe - x = x for all xZx \in \mathbb{Z}. Similarly, the real numbers R\mathbb{R} under subtraction xy=xyx \cdot y = x - y constitute an infinite quasigroup. The operation is closed, and the left and right multiplications are bijective: solving ax=ba - x = b yields x=abx = a - b, and ya=by - a = b yields y=a+by = a + b, with unique solutions in R\mathbb{R}. Like the integer case, it lacks an identity element, rendering it a non-loop quasigroup. This structure extends the additive group (R,+)(\mathbb{R}, +) via conjugation, highlighting how quasigroups can be derived from groups by altering the operation. Vector spaces over fields also yield infinite quasigroups when equipped with componentwise . Consider a VV over a field FF (such as R\mathbb{R} or Q\mathbb{Q}), viewed as FκF^\kappa for some infinite cardinal κ\kappa (e.g., countable ), with the operation (vw)i=viwi(v \cdot w)_i = v_i - w_i for each component index iκi \in \kappa. Since FF under is a quasigroup, the componentwise extension preserves the property: each has a unique componentwise solution, as the operations act independently in each coordinate. This generalizes to arbitrary infinite-dimensional spaces, providing quasigroups of any desired infinite . Free quasigroups offer another fundamental class of infinite examples. The free quasigroup generated by a set XX is the in the variety of quasigroups on the generators XX, constructed as the free extension of the empty partial on XX. For infinite X=λ|X| = \lambda, the of this free quasigroup is λ\lambda, as the terms are finite expressions in the three binary operations (, left division, right division) modulo the quasigroup axioms, yielding a set of size at most λ0=λ\lambda^{\aleph_0} = \lambda under the . These structures are universal objects embedding any map from XX into a quasigroup. Beyond specific constructions, the diversity of infinite quasigroups is vast. For each infinite cardinal λ\lambda, there exist uncountably many pairwise non-isomorphic quasigroups of λ\lambda. This abundance is exemplified in subclasses like Steiner quasigroups, where strongly minimal Steiner triple systems (each coordinatizable by a quasigroup) include uncountably many non-isomorphic models of countable .

Symmetries

Semisymmetry

A quasigroup (Q,)(Q, \cdot) is semisymmetric if it satisfies the identity (xy)x=y(x \cdot y) \cdot x = y for all x,yQx, y \in Q. This condition ensures a form of cyclic symmetry in the multiplication table under the action of the cyclic group C3C_3. Equivalent characterizations include the identity x(yx)=yx \cdot (y \cdot x) = y, or y(xy)=xy \cdot (x \cdot y) = x, or (yx)y=x(y \cdot x) \cdot y = x. In terms of translations, semisymmetry holds if and only if, for every xQx \in Q, the left translation Lx:yxyL_x: y \mapsto x \cdot y and the right translation Rx:yyxR_x: y \mapsto y \cdot x are mutual inverses, satisfying LxRx=idL_x \circ R_x = \mathrm{id} and RxLx=idR_x \circ L_x = \mathrm{id}. Examples of semisymmetric quasigroups include structures derived from abelian groups (G,+)(G, +) equipped with the operation xy=xyx \cdot y = -x - y. For instance, the integers [Z](/page/Z)\mathbb{[Z](/page/Z)} under this operation form an infinite semisymmetric quasigroup. Semisymmetric quasigroups also arise in combinatorial designs, such as extended Mendelsohn triple systems, where blocks correspond to cyclically ordered submultisets of QQ. Semisymmetric quasigroups are flexible, satisfying the identity x(yx)=(xy)xx \cdot (y \cdot x) = (x \cdot y) \cdot x for all x,yQx, y \in Q, since both sides equal yy by the defining identities.

Triality

In quasigroup theory, triality refers to a specific cyclic symmetry in the language of quasigroups, arising from the natural action of the alternating group A3A_3 (the cyclic subgroup of order 3 in S3S_3) on the six parastrophes (conjugate operations) of the quasigroup, preserving the structure under cyclic permutations of the operation symbols. This symmetry is equivalently expressed in binary terms as x/y=yxx / y = y \setminus x for all x,yQx, y \in Q, where // denotes right division and \setminus denotes left division; this equality implies that the left and right division operations coincide after a swap of arguments, reflecting the cyclic interchange. Quasigroups exhibiting triality thus possess a balanced divisibility that aligns the solving mechanisms symmetrically. Examples of quasigroups with triality include commutative Moufang loops of exponent 3, where the operation satisfies x3=ex^3 = e (the identity) for all xx, ensuring the multiplication group admits a triality . Certain Steiner quasigroups, derived from Steiner triple systems and characterized by total (full S3S_3-invariance), also possess triality as a , with the quasigroup operation yielding idempotent, commutative structures where every pair of distinct elements appears uniquely in a "triple." Historically, the concept of triality in algebraic structures like quasigroups draws analogy from Élie Cartan's 1925 introduction of triality for the exceptional of type D4D_4, later connected to the automorphism group of the , which exhibit similar cyclic symmetries in their multiplication; this link has influenced studies of Moufang loops and exceptional geometries arising from quasigroups with triality.

Total Symmetry

A totally symmetric quasigroup is a quasigroup (Q,)(Q, \cdot) in which the relation xy=zx \cdot y = z holds if and only if it holds after any of xx, yy, and zz. Equivalently, for all x,y,zQx, y, z \in Q, xy=zx \cdot y = z implies yx=zy \cdot x = z, xz=yx \cdot z = y, zx=yz \cdot x = y, yz=xy \cdot z = x, and zy=xz \cdot y = x. This condition ensures that all six parastrophes of the quasigroup—the original and the four division operations—coincide as the same on QQ. Consequently, a totally symmetric quasigroup is both commutative, satisfying xy=yxx \cdot y = y \cdot x for all x,yQx, y \in Q, and semi-symmetric, satisfying x(yx)=yx \cdot (y \cdot x) = y for all x,yQx, y \in Q; the latter is a weaker property than total symmetry, as it does not require commutativity. The commutativity of a totally symmetric quasigroup implies that its left multiplication maps La:yayL_a: y \mapsto a \cdot y coincide with its right multiplication maps Ra:yyaR_a: y \mapsto y \cdot a for every aQa \in Q. Moreover, the semi-symmetry condition forces each such map to be an involution, satisfying La2=idQ=Ra2L_a^2 = \mathrm{id}_Q = R_a^2. These symmetries extend to the division operations, making the quasigroup highly symmetric in its . While the variety of totally symmetric quasigroups is defined by these permutation identities, not all members satisfy additional identities such as mediality, (xy)(uv)=(xu)(yv)(x \cdot y) \cdot (u \cdot v) = (x \cdot u) \cdot (y \cdot v), though medial totally symmetric quasigroups form an important subclass with applications in isotopes. Examples of totally symmetric quasigroups include the elementary abelian $2groupsequippedwiththeirgroupoperation;forinstance,theKleinfourgroup-groups equipped with their group operation; for instance, the Klein four-group (\mathbb{Z}/2\mathbb{Z} \times \mathbb{Z}/2\mathbb{Z}, +)satisfiesthetotalsymmetryconditionsbecauseadditionoversatisfies the total symmetry conditions because addition over\mathbb{F}_2iscommutativeandis commutative andx + (y + x) = yholdsduetoholds due to2x = 0.Moregenerally,anyvectorspaceoverthefield. More generally, any vector space over the field \mathbb{F}_2 with componentwise addition yields a totally symmetric quasigroup, providing infinite examples as well. A finite non-group example arises from the cyclic group of order &#36;3 with a modified operation, but such constructions are limited; in fact, the only groups that are totally symmetric quasigroups are precisely the elementary abelian $2$-groups. Totally symmetric idempotent quasigroups, which additionally satisfy xx=xx \cdot x = x for all xQx \in Q, are closely connected to combinatorial designs. Specifically, given such a quasigroup on a set SS, the collection of triples B={{x,y,xy}x,yS,xy}B = \{\{x, y, x \cdot y\} \mid x, y \in S, x \neq y\} forms a Steiner triple system of order S|S|, where every pair from SS appears in exactly one triple. Conversely, every Steiner triple system on SS determines a unique idempotent totally symmetric quasigroup on SS by defining xy=zx \cdot y = z if {x,y,z}\{x, y, z\} is a triple in the system (and xx=xx \cdot x = x). This correspondence links total symmetry to finite geometries and .

Total Antisymmetry

A totally antisymmetric quasigroup, also known as a totally anti-symmetric (TA) quasigroup, is an idempotent quasigroup (Q, ·) in which x · x = x for all x ∈ Q, and the operation is anticommutative in the weak sense that x · y = y · x implies x = y for all x, y ∈ Q. To achieve "total" antisymmetry for applications such as detection, the structure additionally satisfies that for all c, x, y ∈ Q, (c · x) · y = (c · y) · x implies x = y, ensuring that adjacent transpositions alter the result unless the transposed elements are equal. In additive notation, the operation often takes the form x + y ≡ - (y + x) \pmod{n} for finite orders n, reflecting the skew-symmetry of the where entries in symmetric positions sum to 0 n. Such quasigroups exist for every finite order n except n=2 and n=6. These quasigroups are related to anticommutative magmas, where the operation opposes commutativity, and the property aligns with involutory behavior in loop contexts, though TA quasigroups are typically not loops due to the fixed-point-free nature of loop identities. If the quasigroup is a loop with identity e, the generalizes to x · x = e, making the operation involutory and reinforcing the anticommutative structure by ensuring each element is its own inverse in a paired . The division operations in quasigroups provide the unique solvability required for this , as the right division y / x solves y · z = x, linking the antisymmetry to the bijectivity of multiplications. Examples include finite TA quasigroups of order 10 used in the Damm check digit algorithm, where the multiplication table is constructed to satisfy the antisymmetry conditions for error detection in decimal codes. Infinite examples arise in vector spaces equipped with cross product-like operations that can be extended to quasigroup structures in higher odd-dimensional spaces with compatible bilinear forms.

Properties

Multiplication Operators

In a quasigroup (Q,)(Q, \cdot), the left operator by a fixed element aQa \in Q is the map La:QQL_a: Q \to Q defined by La(x)=axL_a(x) = a \cdot x for all xQx \in Q, while the right operator is Ra:QQR_a: Q \to Q given by Ra(x)=xaR_a(x) = x \cdot a. These operators arise naturally from the and capture the action of multiplication from each side. The bijectivity of LaL_a and RaR_a follows directly from the quasigroup axioms, which guarantee unique solvability of the equations ax=ba \cdot x = b and xa=bx \cdot a = b for any bQb \in Q; thus, both maps are permutations of QQ. This property embeds the quasigroup into the Sym(Q)\mathrm{Sym}(Q) via the left ϕL:QSym(Q)\phi_L: Q \to \mathrm{Sym}(Q) given by ϕL(a)=La\phi_L(a) = L_a, and analogously via the right ϕR(a)=Ra\phi_R(a) = R_a. These representations provide a permutation-based view of the quasigroup structure, where the image of ϕL\phi_L (or ϕR\phi_R) acts regularly on QQ. For loops, which are quasigroups equipped with an eQe \in Q satisfying ex=x=xee \cdot x = x = x \cdot e for all xQx \in Q, the operators LeL_e and ReR_e coincide with the identity permutation on QQ, thereby fixing the identity. In general quasigroups (without requiring an identity), the sets {LaaQ}\{L_a \mid a \in Q\} and {RaaQ}\{R_a \mid a \in Q\} generate the translation group of the quasigroup, also termed the multiplication group Mlt(Q)Sym(Q)\mathrm{Mlt}(Q) \leq \mathrm{Sym}(Q), which is the spanned by all left and right multiplications and encodes the transitive action central to quasigroup theory.

Inverse Properties

In quasigroups, the left inverse property (LIP) is defined by the existence of a permutation λ\lambda on the underlying set QQ such that xλ(xy)=yx^\lambda \cdot (x \cdot y) = y for all x,yQx, y \in Q. This condition ensures that left multiplication by xx can be "undone" on the left in a consistent manner, facilitating unique recovery of yy. Analogously, the right inverse property (RIP) holds if there exists a permutation ρ\rho such that (xy)yρ=x(x \cdot y) \cdot y^\rho = x for all x,yQx, y \in Q. These properties strengthen the unique solvability inherent to quasigroups by introducing inverse mappings that align with the binary operation. A loop possessing both the LIP and RIP is termed an inverse property loop (IP-loop), where the permutations λ\lambda and ρ\rho coincide with the two-sided inverse map xx1x \mapsto x^{-1}. In IP-loops, the inverse operation interacts seamlessly with the groupoid structure, leading to identities such as x1(xy)=y=(yx)x1x^{-1} (x y) = y = (y x) x^{-1}. Such loops exhibit enhanced algebraic behavior; for instance, under additional conditions like the Moufang identities, IP-loops are power-associative, meaning that powers xnx^n are well-defined independently of parenthesization for all xQx \in Q and integers nn. Quasigroups inherently satisfy left and right cancellation laws due to their unique solvability: if xy=xzx \cdot y = x \cdot z, then y=zy = z, and similarly for right . These laws follow directly from the existence of unique solutions to the equations xy=bx \cdot y = b and ay=ba \cdot y = b for fixed a,bQa, b \in Q. In the context of inverse properties, cancellation reinforces the invertibility aspects, ensuring that distinct elements remain distinguishable under . The cross inverse property extends these ideas by requiring identities that mix division and multiplication, such as (x\y)z=x\(yz)(x \backslash y) \cdot z = x \backslash (y \cdot z) for all x,y,zQx, y, z \in Q, where \\backslash denotes left division (the unique ww satisfying xw=yx \cdot w = y). Equivalently, this can be expressed via permutations as xyxρ=yx y \cdot x^\rho = y or xyxρ=yx \cdot y x^\rho = y. This captures a form of "crossed" invertibility, where right inverses enable associative-like behavior in divisions, and it holds in structures like cross inverse quasigroups (CIPQs).

Morphisms

Homotopy and Isotopy

In quasigroup theory, a homotopy between two quasigroups (Q,)(Q, \cdot) and (P,)(P, *) is defined as a triple of functions (α,β,γ):QP(\alpha, \beta, \gamma): Q \to P satisfying the equation α(xy)=β(x)γ(y)\alpha(x \cdot y) = \beta(x) * \gamma(y) for all x,yQx, y \in Q. This relation generalizes the notion of a homomorphism by allowing three independent maps rather than a single structure-preserving function, capturing weaker structural similarities between the operations. An isotopy is a special case of a where α\alpha, β\beta, and γ\gamma are all bijective. Isotopy defines an on the class of quasigroups: reflexivity holds via the identity maps, by inverting the bijections, and transitivity by composition of the triples. A principal isotopy occurs when β\beta is the identity map on PP, effectively conjugating the operation by permutations on the left and right factors while fixing the output labeling. Isotopies preserve key structural properties of quasigroups, such as the type defined by identities or the presence of an . Specifically, if (Q,)(Q, \cdot) is a loop (a quasigroup with a two-sided identity), then any quasigroup isotopic to it is also a loop, as the image of the identity under the appropriate serves as the identity in the isotope. Conversely, every quasigroup is isotopic to some loop, allowing the normalization of quasigroups to this form without loss of essential structure. For example, consider two quasigroups on the same finite set corresponding to Latin squares; an isotopism arises from permuting the rows (via β\beta), columns (via γ\gamma), and symbols (via α\alpha) in the multiplication table, yielding isotopic quasigroups with equivalent combinatorial properties. Such transformations demonstrate how isotopy equates quasigroups that differ only in labeling, as seen in the case where a cyclic group quasigroup is principal-isotopic to another via left and right translations.

Parastrophe

In quasigroup theory, a parastrophe of a ⋅ on a set Q is obtained by rearranging the roles of the variables in the defining equation x ⋅ y = z, yielding up to six possible operations corresponding to the permutations of S_3, though for quasigroups these typically reduce to three distinct forms due to the unique solvability of equations. Specifically, given the left division x \ y (the unique z such that x ⋅ z = y) and right division x / y (the unique z such that z ⋅ y = x), the parastrophes include operations defined as x * y = y / x (where y / x is the unique z with z ⋅ x = y), x *' y = x \ y, and x ** y = y \ x (where y \ x is the unique z with y ⋅ z = x). All parastrophes of a quasigroup are themselves quasigroups, as the latin square property is preserved under these rearrangements of the multiplication table. Furthermore, if the original structure is a loop (a quasigroup with identity), each parastrophe retains the loop property, ensuring the existence of a two-sided identity in the new operation. A conjugation of a quasigroup is an isotopy composed with a parastrophe, combining variable permutations with operation rearrangement to relate structures while preserving quasigroup axioms. For example, in the case of groups—which are special quasigroups with associativity and inverses—all parastrophes yield structures isotopic to the original group, and thus isomorphic as groups.

Isostrophe

An isostrophe is defined as the composition of an isotopy and a parastrophe in quasigroup theory, specifically representing an isotopy between two parastrophes of quasigroups. Parastrophes arise from reinterpreting the of a quasigroup (Q,)(Q, \cdot) as one of its five conjugate operations, such as left division x\yx \backslash y or right division y/xy / x, yielding up to six distinct quasigroups associated with the original. An isostrophe thus connects quasigroups that differ both in their underlying permutations (via isotopy) and in the choice of operation (via parastrophe), providing a broader than isotopy alone. Isostrophes preserve additional structural features compared to isotopies, particularly in the groups and properties of quasigroups. For instance, if a loop is an isostrophe of a quasigroup, their middle groups coincide, and the left and right groups of the loop form normal subgroups within this structure. The autotopism group of a quasigroup, which consists of triples of bijections preserving the operation, extends to include isostrophic automorphisms that account for parastrophic rearrangements, enhancing the of symmetries across conjugate operations. In the context of Latin squares, which are equivalent to the multiplication tables of quasigroups, isostrophes correspond to combined manipulations of orthogonal arrays. These include permuting rows, columns, and symbols (from the isotopy component) alongside conjugating the array to reflect a different operation (from the parastrophe), thereby preserving orthogonality properties in sets of mutually orthogonal Latin squares.

Applications

Combinatorics and Design Theory

Quasigroups find prominent applications in combinatorics and design theory through their intimate connection to Latin squares, which are precisely the multiplication tables of finite quasigroups. This bijection allows quasigroup theory to underpin the algebraic study of combinatorial structures like orthogonal arrays and block designs. A historical cornerstone is Euler's 36 officers problem, posed in 1779, which seeks to arrange 36 officers—representing one from each of 6 ranks and 6 regiments—into a 6×6 square such that each row and each column contains exactly one officer from every rank and every regiment. This arrangement is equivalent to constructing two mutually orthogonal Latin squares of order 6, or equivalently, two orthogonal quasigroups of order 6, where orthogonality means that the map sending each pair (x,y)(x, y) to (xy,xy)(x \cdot y, x * y) (with \cdot and * the respective operations) is bijective, ensuring every ordered pair of symbols appears exactly once in the superposition of their tables. Euler conjectured no solution exists for order 6 (or more generally for orders congruent to 2 modulo 4), a claim later confirmed for n=6n=6 by exhaustive enumeration, though disproven for larger such orders. More broadly, sets of (MOLS) of order nn arise from sets of kk mutually orthogonal quasigroups on an nn-element set, where every pair of distinct quasigroups in the set satisfies the condition. Such constructions are central to , enabling the formation of orthogonal arrays OA(n,k+2)(n, k+2) of strength 2, which in turn yield resolvable balanced incomplete block designs and affine geometries. For instance, a complete set of n1n-1 MOLS corresponds to a of order nn, and quasigroup prolongations—extensions preserving Latin square properties—facilitate explicit constructions of orthogonal pairs, as demonstrated for order 10 using T-quasigroups. In the realm of Steiner triple systems, idempotent commutative quasigroups of order v=6n+3v = 6n+3 provide an algebraic model for certain STS(v)(v), which are collections of 3-element blocks on a vv-element set such that every appears in exactly one block. Specifically, a Steiner quasigroup is a totally symmetric idempotent quasigroup satisfying xx=xx \circ x = x, xy=yxx \circ y = y \circ x, and x(yx)=yx(yx) = y; its encodes the triples via xy=zx \circ y = z where {x,y,z}\{x, y, z\} is a block (with z=xz = x if x=yx = y). This equivalence holds isomorphically: STS(v)(v) exist precisely when v1v \equiv 1 or 3(mod6)3 \pmod{6}, and the quasigroup operation uniquely recovers the design, with subsystems corresponding to subquasigroups. Such quasigroups are instrumental in enumerating and constructing large sets of STS, including extensions via idempotent commutative operations. Quasigroup-based error-correcting codes, often derived from transformations, offer robust mechanisms for detecting and correcting errors, including bursts. These nonlinear codes exploit quasigroup operations to generate codewords with low , enabling correction of multiple errors in finite fields; for example, transformations using isotopic quasigroups yield codes with minimum proportional to the quasigroup order. In burst error scenarios, cryptcodes constructed from quasigroups—such as random quasigroup-based encodings—facilitate fast decoding for transmission over noisy channels, correcting contiguous error bursts by leveraging the bijective properties of the operations to recover original data with minimal redundancy. Simulations show these codes achieve bit-error rates comparable to linear codes while resisting adversarial bursts, with performance scaling with quasigroup size.

Cryptography

Quasigroups find significant application in through quasigroup string transformations (QST), which leverage the non-associative to mix input strings in a nonlinear manner, providing a foundation for stream ciphers such as those proposed by Gligoroski et al. in 2004. In these ciphers, QST processes sequences by iteratively applying the quasigroup operation, often combined with over large primes, to generate keystreams that scramble data without relying on associative structures, thereby enhancing diffusion properties. A notable example is the quasigroup encryptor described by Satti et al., which uses indexed quasigroup matrices to achieve high-entropy output even for repetitive inputs, suitable for symmetric stream in resource-constrained environments. Beyond stream ciphers, quasigroups underpin key agreement protocols and hash functions, often via their equivalence to Latin squares. For instance, public-key schemes like Xifrat employ restricted-commutative quasigroups to enable secure key exchange resistant to quantum attacks. Hash functions such as the Edon-R family utilize QST over quasigroups to compress inputs into fixed-length digests, ensuring collision resistance through the quasigroup's permutation properties derived from Latin square representations. A comprehensive 2020 survey by Markovski highlights these uses, noting quasigroups' role in designing primitives for data integrity, digital signatures, and commitment schemes. In 2024, a symmetric encryption scheme based on quasigroups with dynamic S-boxes was proposed, improving resistance to differential and linear cryptanalysis. The non-associativity of quasigroups confers key advantages in , particularly resistance to , as the lack of associative laws prevents straightforward linear approximations of the encryption function. This property disrupts attacks that exploit linearity in group-based ciphers, making quasigroup operations ideal for substitution-permutation networks. Recent developments post-2020 integrate quasigroups into (MPC) protocols, enhancing privacy in distributed systems. For example, a 2025 MPC scheme for resilient coordination selects random elements from quasigroups to perform secure operations like and division, supporting applications in fault-tolerant environments such as networks.

Knot Theory

Quandles, defined as idempotent right-distributive quasigroups satisfying xx=xx \triangleright x = x and (xy)z=(xz)(yz)(x \triangleright y) \triangleright z = (x \triangleright z) \triangleright (y \triangleright z) for all x,y,zx, y, z, provide algebraic invariants for and links. Introduced by Joyce in 1982, quandle colorings assign elements of a quandle to arcs such that the operation respects crossings, distinguishing that groups cannot, such as the and . Quandle homology theories, developed in the 2000s, further enhance these invariants by capturing topological features, with applications in classifying up to concordance and studying link homologies. This connection bridges quasigroup theory with , enabling computational tools for recognition and .

Generalizations

Multiary Quasigroups

A multiary quasigroup, also known as an n-ary quasigroup for n2n \geq 2, is an consisting of a set QQ equipped with an n-ary operation q:QnQq: Q^n \to Q such that, for each position i=1,,ni = 1, \dots, n, the equation q(x1,,xi1,y,xi+1,,xn)=zq(x_1, \dots, x_{i-1}, y, x_{i+1}, \dots, x_n) = z has a unique solution yQy \in Q for any fixed x1,,xi1,xi+1,,xn,zQx_1, \dots, x_{i-1}, x_{i+1}, \dots, x_n, z \in Q. This unique solvability condition generalizes the divisibility property of binary quasigroups to higher arities, ensuring that the operation allows for invertible "divisions" in each variable. When n=2n=2, an n-ary quasigroup reduces precisely to a binary quasigroup, recovering the standard definition with left and right division. For n=3n=3, it yields a ternary quasigroup, where the operation satisfies unique solvability in each of the three positions, often studied for its connections to geometric and combinatorial structures. A key property is reducibility: an n-ary quasigroup is completely reducible if and only if it arises as an iterated binary group operation, such as q(x1,,xn)=x1x2xnq(x_1, \dots, x_n) = x_1 \cdot x_2 \cdots x_n in an , without needing parenthesization to associativity. Examples of multiary quasigroups frequently derive from iterative applications of binary operations. In particular, heaps provide a construction of ternary quasigroups from binary groups or quasigroups: given a group (G,)(G, \cdot) with identity ee, the ternary operation [x,y,z]=xy1z[x, y, z] = x \cdot y^{-1} \cdot z defines a heap, which satisfies the unique solvability condition along with para-associativity [x,y,[z,w,v]]=[[x,y,z],w,v][x, y, [z, w, v]] = [[x, y, z], w, v] and the heap ensuring symmetry in certain divisions. This structure captures "group-like" behavior without a specified identity, and its retracts (by fixing one variable) often yield binary quasigroups. Recent advancements extend multiary quasigroups to hyperstructural settings through polyquasigroups and polylops, introduced in 2025. A polyquasigroup is a polygroupoid—a set with a hyperoperation producing subsets—equipped with hyperdivisions satisfying inclusion-based solvability conditions, such as x(xy)/yx \in (x \cdot y) / y for all x,yx, y, generalizing unique solvability to multi-valued outputs. A polylop further requires a hyperidentity ee such that xe=ex=xx \cdot e = e \cdot x = x. Examples include finite sets like {1,2,3,4,5,6,7}\{1,2,3,4,5,6,7\} with explicitly tabulated hyperoperations forming polyquasigroups, and subsets thereof yielding polylops with identity 1, illustrating applications in hypergroup theory and generalized algebraic systems.

Quasigroupoids

A quasigroupoid is a of a to non-associative settings, often defined in categorical terms as a magmoid where every span and cospan admits a unique . In algebraic terms, as studied in recent work, a quasigroupoid QI\mathcal{Q} \rightrightarrows \mathcal{I} consists of a set QI\mathcal{Q} \supset \mathcal{I} (with I\mathcal{I} \neq \emptyset) equipped with partial binary and inversion, source σ:QI\sigma: \mathcal{Q} \to \mathcal{I}, and target τ:QI\tau: \mathcal{Q} \to \mathcal{I}, such that multiplication is defined only when τ(x)=σ(y)\tau(x) = \sigma(y), with associativity holding whenever defined, every element having an inverse, and appropriate identity conditions via the maps. This structure ensures local solvability properties akin to quasigroups but in a partial, directed setting. Quasigroupoids generalize quasigroups by relaxing the totality of the operation and incorporating categorical structure, allowing undefined products while maintaining divisibility where defined. They encompass loopoids as a subclass, which are partial loops featuring a partial satisfying ex=xe=xe \cdot x = x \cdot e = x whenever defined. Examples of quasigroupoids include partial Latin squares, where the defined entries form a satisfying the local quasigroup axioms, with undefined cells representing non-computable products. They also appear in incomplete block designs, where the partial operation encodes incidence relations that are not specified for every pair of elements, yet satisfy solvability for defined blocks. Recent developments, published online in January 2025, introduced matrix representations for quasigroupoids, generalizing classical matrix models of groupoids to non-associative contexts by employing a parameterized family of quasigroups Θ(P,I)\Theta(\mathcal{P}, \mathcal{I}) with source σ\sigma and target τ\tau maps to define partial multiplications, such as (h,x,j)(k,y,l)=(h,θhjl(x,y),l)(h, x, j) \cdot (k, y, l) = (h, \theta_{hjl}(x, y), l) when j=kj = k. This approach proves that every connected quasigroupoid admits a non-canonical matrix representation (Theorem 5), facilitating the study of their embeddings and decompositions, including loopoids into pair groupoids and loops.

Enumeration

Small Quasigroups

The enumeration of quasigroups of small finite orders up to reveals a rapid increase in complexity even for modest sizes. For order 1, there is a single trivial quasigroup on the singleton set, where the operation maps the unique element to itself. For order 2, there is exactly one quasigroup up to , which coincides with the of order 2 and thus is a loop. For order 3, there are five quasigroups up to , of which one is a loop (the of order 3). These five arise from the 12 Latin squares of order 3, classified into isomorphism classes via their Cayley tables. For order 4, there are 35 quasigroups up to , including two loops (the of order 4 and the ). The classification into these 35 classes was obtained by enumerating the 576 Latin squares of order 4 and grouping them by quasigroup isomorphisms, which preserve the . The following table summarizes the counts of quasigroups and loops up to for orders 1 through 4:
OrderQuasigroupsLoops
111
211
351
4352
The growth in the number of quasigroups of order nn up to is tracked by OEIS sequence A057991, with values 1, 1, 5, 35, 1411, 1130531 for n=1n = 1 to 6, illustrating that renders complete enumeration computationally intensive beyond small nn. These enumerations were computed using orderly generation techniques and tools such as nauty to determine canonical forms and classes from representations. The GAP package LOOPS further facilitates such computations for quasigroups and loops of small orders by integrating methods and libraries for nonassociative structures.

Small Loops

The enumeration and classification of small finite loops up to focus on their structure as quasigroups with a two-sided . For orders 1 through 3, there is precisely one loop of each order, and each is associative, coinciding with the Zn\mathbb{Z}_n. Specifically, the loop of order 1 is the , that of order 2 is Z2\mathbb{Z}_2, and that of order 3 is Z3\mathbb{Z}_3. For order 4, there are two non-isomorphic loops, both associative and thus groups: the Z4\mathbb{Z}_4 and the Z2×Z2\mathbb{Z}_2 \times \mathbb{Z}_2 (also known as the of order 4). It is a known result that all loops of order at most 4 are associative. Non-associative loops first appear at order 5, where there are six loops up to : one associative loop, the Z5\mathbb{Z}_5, and five non-associative examples. The complete counts of loops up to for small orders are summarized in the following table:
Order nnNumber of loops up to
11
21
31
42
56
These enumerations distinguish associative loops (groups) from non-associative ones, highlighting the scarcity of non-associative structures in very small orders. The sequence of the number of loops of order nn up to is cataloged as OEIS A057771.

References

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