Nonassociative algebras

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Let AA be an algebra with identity 1 over R\mathbb {R}. Let a conjugation operation x↦xˉx \mapsto \bar{x} be given on AA, possessing the properties xˉ‾=x,xy‾=yx‾\overline{\bar{x}}=x, \overline{x y}=\overline{y x}. Let us equip the space A⊕A={(x,y)∣x,y∈A}A \oplus A=\left\{ (x, y) \mid x, y \in A\right\} with the bilinear multiplication operation

(x,y)(u,v)=(xu−vˉy,yuˉ+vx) (x, y)(u, v)=(x u-\bar{v} y, y \bar{u}+v x)

One obtains an algebra called the doubling of the algebra AA.

Verify that C\mathbb {C} is the doubling of the algebra R\mathbb {R}, and H\mathbb {H} the doubling of the algebra C\mathbb {C}. The doubling of the algebra H\mathbb {H} is called the Cayley algebra Ca\mathrm{Ca}.

Verify that Ca\mathrm{Ca} is a noncommutative and nonassociative algebra. Express explicitly the conjugation operation on Ca\mathrm{Ca}.

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Consider F2n\mathbb {F}_{2^{n}} as a vector space VV of dimension nn over F2\mathbb {F}_{2}. Alongside the addition operation inherited from F2n\mathbb {F}_{2^{n}}, introduce on VV the multiplication operation (x,y)↦x∘y=xy(x, y) \mapsto x \circ y=\sqrt{x y}. Here x↦xx \mapsto \sqrt{x} is the automorphism of F2n\mathbb {F}_{2^{n}} inverse to x↦x2x \mapsto x^{2}, so that x+y=x+y\sqrt{x+y}=\sqrt{x}+\sqrt{y}. Show that (V,+,∘)(V,+, \circ ) is a commutative (nonassociative) algebra over F2\mathbb {F}_{2}, possessing the properties:

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(a)

VV has no zero divisors and no identity;

(b)

the equation a∘x=ba \circ x=b with a≠0a \neq 0 is uniquely solvable;

(c)

the automorphism group Aut⁡(V)\operatorname {Aut}(V) acts transitively on V\{0}V \backslash \left\{ 0\right\}.

In any algebra the identity for associators holds

t(x,y,z)+(t,x,y)z=(tx,y,z)−(t,xy,z)+(t,x,yz) t(x, y, z)+(t, x, y) z=(t x, y, z)-(t, x y, z)+(t, x, y z)

Verify this by direct checking, and show that if, in an algebra AA with identity 1 over a field PP, the inclusion (x,y,z)∈P⋅1(x, y, z) \in P \cdot 1 holds for all associators, then AA is an associative algebra.

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The octonion algebra O\mathcal{O} is an 8-dimensional non-associative algebra. It is defined in terms of the basis elements eμe_{\mu } (μ=0,1,…,7\mu = 0, 1, \ldots , 7) and their multiplication table. e0e_{0} is the unit element. We use Greek indices (μ,ν,…)(\mu , \nu , \ldots ) to include the 0 and latin indices (i,j,k,…)(i, j, k, \ldots ) when we exclude the 0. We define

e^k:=e4+kfork=1,2,3. \hat{e}_{k} := e_{4+k} \quad \text{for} \quad k = 1, 2, 3.

The multiplication rules among the basis elements of octonions eμe_{\mu } are given by

eiej=−δije0+∑k=13ϵijkek,i,j,k=1,2,3(1) e_{i}e_{j} = -\delta _{ij}e_{0} + \sum _{k=1}^{3} \epsilon _{ijk}e_{k}, \qquad i, j, k = 1, 2, 3 \tag {1}

and

−e4ei=eie4=e^i,e4e^i=−e^ie4=ei,e4e4=−e0 -e_{4}e_{i} = e_{i}e_{4} = \hat{e}_{i}, \qquad e_{4}\hat{e}_{i} = -\hat{e}_{i}e_{4} = e_{i}, \qquad e_{4}e_{4} = -e_{0} e^ie^j=−δije0−∑k=13ϵijkek,i,j,k=1,2,3 \hat{e}_{i}\hat{e}_{j} = -\delta _{ij}e_{0} - \sum _{k=1}^{3} \epsilon _{ijk}e_{k}, \qquad i, j, k = 1, 2, 3 −e^jei=eie^j=−δije4−∑k=13ϵijke^k,i,j,k=1,2,3 -\hat{e}_{j}e_{i} = e_{i}\hat{e}_{j} = -\delta _{ij}e_{4} - \sum _{k=1}^{3} \epsilon _{ijk}\hat{e}_{k}, \qquad i, j, k = 1, 2, 3

where δij\delta_{ij} is the Kronecker delta and ϵijk\epsilon_{ijk} is +1+1 if (ijk)(ijk) is an even permutation of (123)(123), −1-1 if (ijk)(ijk) is an odd permutation of (123)(123) and 0 otherwise. We can formally summarize the multiplications as

eμeν=gμνe0+∑k=17γμνkek e_{\mu }e_{\nu } = g_{\mu \nu }e_{0} + \sum _{k=1}^{7} \gamma _{\mu \nu }^{k}e_{k}

where

gμν=diag⁡(1,−1,−1,−1,−1,−1,−1,−1),γijk=−γjik g_{\mu \nu } = \operatorname {diag}(1, -1, -1, -1, -1, -1, -1, -1), \qquad \gamma _{ij}^{k} = -\gamma _{ji}^{k}

with μ,ν=0,1,…,7\mu , \nu = 0, 1, \ldots , 7, and i,j,k=1,2,…,7i, j, k = 1, 2, \ldots , 7.

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(i)

Show that the set {e0,e1,e2,e3}\left\{ e_{0}, e_{1}, e_{2}, e_{3}\right\} is a closed associative subalgebra.

(ii)

Show that the octonian algebra O\mathcal{O} is non-associative.

Consider the vector space R3\mathbb {R}^{3} and the vector product ×\times. The vector product is not associative. The associator of three vectors u→\overrightarrow {u}, v→\overrightarrow {v}, w→\overrightarrow {w} is defined by

ass⁡(u→×(v→×w→)):=(u→×v→)×w→−u→×(v→×w→). \operatorname {ass}(\overrightarrow {u} \times (\overrightarrow {v} \times \overrightarrow {w})) := (\overrightarrow {u} \times \overrightarrow {v}) \times \overrightarrow {w} - \overrightarrow {u} \times (\overrightarrow {v} \times \overrightarrow {w}).

The associator measures the failure of associativity.

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(i)

Consider the unit vectors

u→=(100),v→=(010),w→=(001). \overrightarrow {u} = \begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix}, \qquad \overrightarrow {v} = \begin{pmatrix} 0 \\ 1 \\ 0 \end{pmatrix}, \qquad \overrightarrow {w} = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix}.

Find the associator.

(ii)

Consider the normalized vectors

u→=12(101),v→=(010),w→=12(10−1). \overrightarrow {u} = \frac{1}{\sqrt{2}}\begin{pmatrix} 1 \\ 0 \\ 1 \end{pmatrix}, \qquad \overrightarrow {v} = \begin{pmatrix} 0 \\ 1 \\ 0 \end{pmatrix}, \qquad \overrightarrow {w} = \frac{1}{\sqrt{2}}\begin{pmatrix} 1 \\ 0 \\ -1 \end{pmatrix}.

Find the associator.

References

[Кос04] Кострикин А.И. Основные структуры алгебры. ФИЗМАТЛИТ, 2004.
[StHa17] Steeb W., Hardy Y. Problems and Solutions in Introductory and Advanced Matrix Calculus. 2nd ed., World Scientific Publishing, 2017.
[Вин14] Винберг Э.Б. Курс алгебры. 2-е изд., МЦНМО, 2014.