133 lines
9.0 KiB
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133 lines
9.0 KiB
Plaintext
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[1X2 [33X[0;0YMathematical Background[133X[101X
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[33X[0;0YWe assume that you are familiar with the theory of quasigroups and loops,
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for instance with the textbook of Bruck [Bru58] or Pflugfelder [Pfl90].
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Nevertheless, we did include definitions and results in this manual in order
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to unify terminology and improve legibility of the text. Some general
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concepts of quasigroups and loops can be found in this chapter. More special
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concepts are defined throughout the text as needed.[133X
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[1X2.1 [33X[0;0YQuasigroups and Loops[133X[101X
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[33X[0;0YA set with one binary operation (denoted [22X⋅[122X here) is called [13Xgroupoid[113X or
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[13Xmagma[113X, the latter name being used in [5XGAP[105X.[133X
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[33X[0;0YAn element [22X1[122X of a groupoid [22XG[122X is a [13Xneutral element[113X or an [13Xidentity element[113X if
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[22X1⋅ x = x⋅ 1 = x[122X for every [22Xx[122X in [22XG[122X.[133X
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[33X[0;0YLet [22XG[122X be a groupoid with neutral element [22X1[122X. Then an element [22Xx^-1[122X is called a
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[13Xtwo-sided inverse[113X of [22Xx[122X in [22XG[122X if [22Xx⋅ x^-1 = x^-1⋅ x = 1[122X.[133X
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[33X[0;0YRecall that groups are associative groupoids with an identity element and
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two-sided inverses. Groups can be reached in another way from groupoids,
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namely via quasigroups and loops.[133X
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[33X[0;0YA [13Xquasigroup[113X [22XQ[122X is a groupoid such that the equation [22Xx⋅ y=z[122X has a unique
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solution in [22XQ[122X whenever two of the three elements [22Xx[122X, [22Xy[122X, [22Xz[122X of [22XQ[122X are specified.
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Note that multiplication tables of finite quasigroups are precisely [13Xlatin
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squares[113X, i.e., square arrays with symbols arranged so that each symbol
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occurs in each row and in each column exactly once. A [13Xloop[113X [22XL[122X is a quasigroup
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with a neutral element.[133X
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[33X[0;0YGroups are clearly loops. Conversely, it is not hard to show that
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associative quasigroups are groups.[133X
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[1X2.2 [33X[0;0YTranslations[133X[101X
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[33X[0;0YGiven an element [22Xx[122X of a quasigroup [22XQ[122X, we can associative two permutations of
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[22XQ[122X with it: the [13Xleft translation[113X [22XL_x:Q-> Q[122X defined by [22Xy↦ x⋅ y[122X, and the [13Xright
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translation[113X [22XR_x:Q-> Q[122X defined by [22Xy↦ y⋅ x[122X.[133X
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[33X[0;0YThe binary operation [22Xxbackslash y = L_x^-1(y)[122X is called the [13Xleft division[113X,
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and [22Xx/y = R_y^-1(x)[122X is called the [13Xright division[113X.[133X
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[33X[0;0YAlthough it is possible to compose two left (right) translations of a
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quasigroup, the resulting permutation is not necessarily a left (right)
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translation. The set [22X{L_x|x∈ Q}[122X is called the [13Xleft section[113X of [22XQ[122X, and [22X{R_x|x∈
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Q}[122X is the [13Xright section[113X of [22XQ[122X.[133X
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[33X[0;0YLet [22XS_Q[122X be the symmetric group on [22XQ[122X. Then the subgroup [22XMlt_λ(Q)=⟨ L_x|x∈ Q⟩[122X
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of [22XS_Q[122X generated by all left translations is the [13Xleft multiplication group[113X
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of [22XQ[122X. Similarly, [22XMlt_ρ(Q)= ⟨ R_x|x∈ Q⟩[122X is the [13Xright multiplication group[113X of
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[22XQ[122X. The smallest group containing both [22XMlt_λ(Q)[122X and [22XMlt_ρ(Q)[122X is called the
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[13Xmultiplication group[113X of [22XQ[122X and is denoted by [22XMlt(Q)[122X.[133X
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[33X[0;0YFor a loop [22XQ[122X, the [13Xleft inner mapping group[113X [22XInn_λ(Q)[122X is the stabilizer of [22X1[122X
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in [22XMlt_λ(Q)[122X. The [13Xright inner mapping group[113X [22XInn_ρ(Q)[122X is defined dually. The
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[13Xinner mapping group[113X [22XInn(Q)[122X is the stabilizer of [22X1[122X in [22XQ[122X.[133X
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[1X2.3 [33X[0;0YSubquasigroups and Subloops[133X[101X
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[33X[0;0YA nonempty subset [22XS[122X of a quasigroup [22XQ[122X is a [13Xsubquasigroup[113X if it is closed
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under multiplication and the left and right divisions. In the finite case,
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it suffices for [22XS[122X to be closed under multiplication. [13XSubloops[113X are defined
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analogously when [22XQ[122X is a loop.[133X
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[33X[0;0YThe [13Xleft nucleus[113X [22XNuc_λ(Q)[122X of [22XQ[122X consists of all elements [22Xx[122X of [22XQ[122X such that
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[22Xx(yz) = (xy)z[122X for every [22Xy[122X, [22Xz[122X in [22XQ[122X. The [13Xmiddle nucleus[113X [22XNuc_μ(Q)[122X and the [13Xright
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nucleus[113X [22XNuc_ρ(Q)[122X are defined analogously. The [13Xnucleus[113X [22XNuc(Q)[122X is the
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intersection of the left, middle and right nuclei.[133X
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[33X[0;0YThe [13Xcommutant[113X [22XC(Q)[122X of [22XQ[122X consists of all elements [22Xx[122X of [22XQ[122X that commute with
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all elements of [22XQ[122X. The [13Xcenter[113X [22XZ(Q)[122X of [22XQ[122X is the intersection of [22XNuc(Q)[122X with
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[22XC(Q)[122X.[133X
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[33X[0;0YA subloop [22XS[122X of [22XQ[122X is [13Xnormal[113X in [22XQ[122X if [22Xf(S)=S[122X for every inner mapping [22Xf[122X of [22XQ[122X.[133X
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[1X2.4 [33X[0;0YNilpotence and Solvability[133X[101X
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[33X[0;0YFor a loop [22XQ[122X define [22XZ_0(Q) = 1[122X and let [22XZ_i+1(Q)[122X be the preimage of the
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center of [22XQ/Z_i(Q)[122X in [22XQ[122X. A loop [22XQ[122X is [13Xnilpotent of class[113X [22Xn[122X if [22Xn[122X is the least
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nonnegative integer such that [22XZ_n(Q)=Q[122X. In such case [22XZ_0(Q)le Z_1(Q)le dots
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le Z_n(Q)[122X is the [13Xupper central series[113X.[133X
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[33X[0;0YThe [13Xderived subloop[113X [22XQ'[122X of [22XQ[122X is the least normal subloop of [22XQ[122X such that [22XQ/Q'[122X
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is a commutative group. Define [22XQ^(0)=Q[122X and let [22XQ^(i+1)[122X be the derived
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subloop of [22XQ^(i)[122X. Then [22XQ[122X is [13Xsolvable of class[113X [22Xn[122X if [22Xn[122X is the least
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nonnegative integer such that [22XQ^(n) = 1[122X. In such a case [22XQ^(0)ge Q^(1)ge ⋯ ge
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Q^(n)[122X is the [13Xderived series[113X of [22XQ[122X.[133X
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[1X2.5 [33X[0;0YAssociators and Commutators[133X[101X
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[33X[0;0YLet [22XQ[122X be a quasigroup and let [22Xx[122X, [22Xy[122X, [22Xz[122X be elements of [22XQ[122X. Then the [13Xcommutator[113X
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of [22Xx[122X, [22Xy[122X is the unique element [22X[x,y][122X of [22XQ[122X such that [22Xxy = [x,y](yx)[122X, and the
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[13Xassociator[113X of [22Xx[122X, [22Xy[122X, [22Xz[122X is the unique element [22X[x,y,z][122X of [22XQ[122X such that [22X(xy)z =
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[x,y,z](x(yz))[122X.[133X
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[33X[0;0YThe [13Xassociator subloop[113X [22XA(Q)[122X of [22XQ[122X is the least normal subloop of [22XQ[122X such that
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[22XQ/A(Q)[122X is a group.[133X
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[33X[0;0YIt is not hard to see that [22XA(Q)[122X is the least normal subloop of [22XQ[122X containing
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all commutators, and [22XQ'[122X is the least normal subloop of [22XQ[122X containing all
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commutators and associators.[133X
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[1X2.6 [33X[0;0YHomomorphism and Homotopisms[133X[101X
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[33X[0;0YLet [22XK[122X, [22XH[122X be two quasigroups. Then a map [22Xf:K-> H[122X is a [13Xhomomorphism[113X if [22Xf(x)⋅
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f(y)=f(x⋅ y)[122X for every [22Xx[122X, [22Xy∈ K[122X. If [22Xf[122X is also a bijection, we speak of an
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[13Xisomorphism[113X, and the two quasigroups are called isomorphic.[133X
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[33X[0;0YAn ordered triple [22X(α,β,γ)[122X of maps [22Xα[122X, [22Xβ[122X, [22Xγ:K-> H[122X is a [13Xhomotopism[113X if [22Xα(x)⋅β(y)
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= γ(x⋅ y)[122X for every [22Xx[122X, [22Xy[122X in [22XK[122X. If the three maps are bijections, then
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[22X(α,β,γ)[122X is an [13Xisotopism[113X, and the two quasigroups are isotopic.[133X
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[33X[0;0YIsotopic groups are necessarily isomorphic, but this is certainly not true
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for nonassociative quasigroups or loops. In fact, every quasigroup is
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isotopic to a loop.[133X
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[33X[0;0YLet [22X(K,⋅)[122X, [22X(K,∘)[122X be two quasigroups defined on the same set [22XK[122X. Then an
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isotopism [22X(α,β, id_K)[122X is called a [13Xprincipal isotopism[113X. An important class of
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principal isotopisms is obtained as follows: Let [22X(K,⋅)[122X be a quasigroup, and
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let [22Xf[122X, [22Xg[122X be elements of [22XK[122X. Define a new operation [22X∘[122X on [22XK[122X by [22Xx∘ y =
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R_g^-1(x)⋅ L_f^-1(y)[122X, where [22XR_g[122X, [22XL_f[122X are translations. Then [22X(K,∘)[122X is a
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quasigroup isotopic to [22X(K,⋅)[122X, in fact a loop with neutral element [22Xf⋅ g[122X. We
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call [22X(K,∘)[122X a [13Xprincipal loop isotope[113X of [22X(K,⋅)[122X.[133X
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