Difference between revisions of "Algebra with associative powers"
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− | A linear algebra | + | A linear algebra $A$ over a field $F$ each element of which generates an associative subalgebra. The set of all algebras with associative powers over a given field $F$ forms a variety of algebras which, if the characteristic of the field $F$ is zero, is defined by the system of identities |
+ | $$\label{1} | ||
+ | (x,x,x) = (x^2,x,x) = 0 | ||
+ | $$ | ||
+ | where the [[associator]] $(a,b,c) = (ab)c - a(bc)$. If $F$ is an infinite field of prime characteristic $p$, then the variety of algebras with associative powers cannot be defined by any finite system of identities, but an independent, infinite system of identities which defines it is known [[#References|[3]]]. If a commutative algebra $A$ with associative powers of characteristic other than $2$ has an idempotent $e \neq 0$, then $A$ can be decomposed according to Peirce into a direct sum of vector subspaces: | ||
+ | $$\label{2} | ||
+ | A = A_0(e) \oplus A_{\frac12}(e) \oplus A_1(e) | ||
+ | $$ | ||
+ | where $A_\lambda(e) = \{ a \in A : ea = \lambda a \}$, $\lambda = 0,\frac12,1$. Here $A_0(e)$ and $A_1(e)$ are subalgebras, $A_0(e) A_1(e) = 0$, $A_{\frac12}(e)A_{\frac12}(e) \subseteq A_0(e) + A_1(e)$, $A_\lambda(e) A_{\frac12}(e) \subseteq A_{\frac12}(e) + A_{1-\lambda}(e)$ for $\lambda = 0,1$. The Pierce decomposition (2) plays a fundamental role in the structure theory of algebras with associative powers. | ||
− | <table | + | ====References==== |
+ | <table> | ||
+ | <TR><TD valign="top">[1]</TD> <TD valign="top"> A.A. Albert, "Power-associative rings" ''Trans. Amer. Math. Soc.'' , '''64''' (1948) pp. 552–593</TD></TR> | ||
+ | <TR><TD valign="top">[2]</TD> <TD valign="top"> A.T. Gainov, "Identity relations for binary Lie rings" ''Uspekhi Mat. Nauk'' , '''12''' : 3 (1957) pp. 141–146 (In Russian)</TD></TR> | ||
+ | <TR><TD valign="top">[3]</TD> <TD valign="top"> A.T. Gainov, "Power-associative algebras over a finite-characteristic field" ''Algebra and Logic'' , '''9''' : 1 (1970) pp. 5–19 ''Algebra i Logika'' , '''9''' : 1 (1970) pp. 9–33</TD></TR> | ||
+ | </table> | ||
− | + | ====Comments==== | |
− | + | An algebra with associative powers is also called a power-associative algebra. The fact that the set of algebras with associative powers over a field of non-zero characteristic forms a variety defined by | |
− | + | (1) $(x,x,x) = (x^2,x,x) = 0$ | |
− | + | was proved in {{Cite|a1}}. | |
− | |||
====References==== | ====References==== | ||
− | |||
− | |||
− | |||
− | + | * {{Ref|a1}} A.A. Albert, "On the power associativity of rings" ''Summa Brasiliensis Math.'' , '''2''' (1948) pp. 21–33 {{ZBL|0039.26403}} | |
− | |||
− | + | {{TEX|done}} | |
− |
Latest revision as of 10:19, 16 March 2023
A linear algebra $A$ over a field $F$ each element of which generates an associative subalgebra. The set of all algebras with associative powers over a given field $F$ forms a variety of algebras which, if the characteristic of the field $F$ is zero, is defined by the system of identities $$\label{1} (x,x,x) = (x^2,x,x) = 0 $$ where the associator $(a,b,c) = (ab)c - a(bc)$. If $F$ is an infinite field of prime characteristic $p$, then the variety of algebras with associative powers cannot be defined by any finite system of identities, but an independent, infinite system of identities which defines it is known [3]. If a commutative algebra $A$ with associative powers of characteristic other than $2$ has an idempotent $e \neq 0$, then $A$ can be decomposed according to Peirce into a direct sum of vector subspaces: $$\label{2} A = A_0(e) \oplus A_{\frac12}(e) \oplus A_1(e) $$ where $A_\lambda(e) = \{ a \in A : ea = \lambda a \}$, $\lambda = 0,\frac12,1$. Here $A_0(e)$ and $A_1(e)$ are subalgebras, $A_0(e) A_1(e) = 0$, $A_{\frac12}(e)A_{\frac12}(e) \subseteq A_0(e) + A_1(e)$, $A_\lambda(e) A_{\frac12}(e) \subseteq A_{\frac12}(e) + A_{1-\lambda}(e)$ for $\lambda = 0,1$. The Pierce decomposition (2) plays a fundamental role in the structure theory of algebras with associative powers.
References
[1] | A.A. Albert, "Power-associative rings" Trans. Amer. Math. Soc. , 64 (1948) pp. 552–593 |
[2] | A.T. Gainov, "Identity relations for binary Lie rings" Uspekhi Mat. Nauk , 12 : 3 (1957) pp. 141–146 (In Russian) |
[3] | A.T. Gainov, "Power-associative algebras over a finite-characteristic field" Algebra and Logic , 9 : 1 (1970) pp. 5–19 Algebra i Logika , 9 : 1 (1970) pp. 9–33 |
Comments
An algebra with associative powers is also called a power-associative algebra. The fact that the set of algebras with associative powers over a field of non-zero characteristic forms a variety defined by (1) $(x,x,x) = (x^2,x,x) = 0$ was proved in [a1].
References
- [a1] A.A. Albert, "On the power associativity of rings" Summa Brasiliensis Math. , 2 (1948) pp. 21–33 Zbl 0039.26403
Algebra with associative powers. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Algebra_with_associative_powers&oldid=16404