Power-associative algebras relax associativity while maintaining certain power-related properties. They bridge the gap between associative and fully non-associative structures, allowing for well-defined powers without full associativity.
These algebras include octonions , Jordan algebras, and flexible algebras. They satisfy key identities like the fourth-degree condition and have important relationships with other algebraic structures, subalgebras, and ideals.
Definition of power-associative algebras
Non-associative algebras form the broader context for power-associative algebras in algebraic structures
Power-associative algebras relax the associativity condition while maintaining certain power-related properties
Crucial concept in Non-associative Algebra bridges the gap between associative and fully non-associative structures
Key properties
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Powers of elements associate regardless of parenthesization
Satisfies the identity ( x m ) [ x n ] ( h t t p s : / / w w w . f i v e a b l e K e y T e r m : x n ) = x m + n (x^m)[x^n](https://www.fiveableKeyTerm:x^n) = x^{m+n} ( x m ) [ x n ] ( h ttp s : // www . f i v e ab l eKey T er m : x n ) = x m + n for all positive integers m and n
Allows for well-defined notion of powers without full associativity
Generalizes associative algebras while maintaining some computational convenience
Includes both associative and some non-associative algebras as special cases
Algebraic structure
Defined over a field or ring, typically denoted as F
Vector space structure with an additional bilinear multiplication operation
Multiplication not necessarily associative or commutative
Closure property ensures product of any two elements remains in the algebra
Identity element may or may not exist, depending on the specific algebra
Examples of power-associative algebras
Power-associative algebras encompass a wide range of algebraic structures
Studying examples helps illuminate the diversity and applications of these algebras
Crucial for understanding the broader landscape of Non-associative Algebra
Octonions
Non-associative division algebra over the real numbers
8-dimensional algebra with a basis of 8 unit octonions
Satisfies power-associativity but not full associativity
Generalizes complex numbers and quaternions
Applications in theoretical physics (string theory, M-theory)
Multiplication table defines the octonion product
Jordan algebras
Commutative power-associative algebras
Satisfy the Jordan identity: ( x 2 y ) x = x 2 ( y x ) (x^2y)x = x^2(yx) ( x 2 y ) x = x 2 ( y x )
Originally developed to formalize quantum mechanics observables
Special Jordan algebras derived from associative algebras
Exceptional Jordan algebras not derived from associative algebras (Albert algebras)
Connection to projective geometry and quantum information theory
Flexible algebras
Satisfy the flexibility condition: ( x y ) x = x ( y x ) (xy)x = x(yx) ( x y ) x = x ( y x ) for all elements x and y
Generalize associative and alternative algebras
Include Lie-admissible algebras as a subclass
Power-associativity follows from flexibility in characteristic ≠ 2, 3
Examples include Jordan algebras and some genetic algebras
Power-associativity conditions
Conditions defining power-associative algebras form the foundation of their theory
Understanding these conditions essential for analyzing and classifying power-associative structures
Crucial concept in Non-associative Algebra for generalizing associativity
Degree conditions
Third-degree condition: ( x x ) x = x ( x x ) (xx)x = x(xx) ( xx ) x = x ( xx ) for all elements x
Fourth-degree condition: ( x x ) ( x x ) = ( x ( x x ) ) x (xx)(xx) = (x(xx))x ( xx ) ( xx ) = ( x ( xx )) x for all elements x
Higher-degree conditions ensure consistency of powers beyond the fourth power
Sufficient conditions for power-associativity in characteristic 0 or sufficiently large
Interplay between degree conditions and characteristic of the base field
Linearization techniques
Method to derive equivalent conditions by replacing variables with linear combinations
Allows for the study of power-associativity using multilinear identities
Partial linearization replaces some occurrences of a variable
Full linearization replaces all occurrences of a variable
Useful for proving theorems and deriving new identities in power-associative algebras
Relation to other algebras
Power-associative algebras occupy a unique position in the hierarchy of algebraic structures
Understanding their relationships to other algebra types crucial for broader context in Non-associative Algebra
Comparisons highlight the distinctive features and generalizations of power-associative algebras
vs Associative algebras
Associative algebras form a proper subclass of power-associative algebras
Power-associative algebras relax the full associativity condition
Associative algebras satisfy ( a b ) c = a ( b c ) (ab)c = a(bc) ( ab ) c = a ( b c ) for all elements a, b, c
Power-associative algebras only require associativity for powers of the same element
Examples of power-associative algebras that are not associative (octonions, Jordan algebras)
vs Alternative algebras
Alternative algebras satisfy ( x x ) y = x ( x y ) (xx)y = x(xy) ( xx ) y = x ( x y ) and ( y x ) x = y ( x x ) (yx)x = y(xx) ( y x ) x = y ( xx ) for all elements x, y
All alternative algebras are power-associative, but not vice versa
Alternative algebras include associative algebras and octonions
Power-associative algebras allow for more general structures than alternative algebras
Flexibility holds in alternative algebras but not necessarily in all power-associative algebras
Power-associative identities
Identities characterize and define the behavior of power-associative algebras
Understanding these identities crucial for proving theorems and analyzing structures
Form the foundation for studying power-associative algebras in Non-associative Algebra
Fourth-degree identity
Fundamental identity for power-associative algebras: ( x x ) ( x x ) = ( x ( x x ) ) x (xx)(xx) = (x(xx))x ( xx ) ( xx ) = ( x ( xx )) x
Ensures consistency of the fourth power regardless of parenthesization
Equivalent to the condition that all polynomials of degree 4 in one variable associate
Can be derived from third-degree associativity in characteristic ≠ 2, 3
Plays a crucial role in the classification of power-associative algebras
Higher-degree identities
Generalize the fourth-degree identity to higher powers
Ensure consistency of all powers beyond the fourth power
Can be expressed as multilinear identities through linearization techniques
Examples include fifth-degree identity: ( ( x x ) x ) ( x x ) = ( x x ) ( ( x x ) x ) ((xx)x)(xx) = (xx)((xx)x) (( xx ) x ) ( xx ) = ( xx ) (( xx ) x )
Higher-degree identities become increasingly complex and challenging to verify
Subalgebras and ideals
Subalgebras and ideals form essential building blocks for understanding algebraic structures
Studying these substructures crucial for analyzing and classifying power-associative algebras
Important concepts in Non-associative Algebra for decomposing and constructing algebras
Power-associative subalgebras
Subalgebras of power-associative algebras that maintain power-associativity
Closed under addition, scalar multiplication, and algebra multiplication
Generated by a single element (one-generated subalgebras always power-associative)
May possess additional properties not present in the parent algebra
Examples include the real subalgebra of octonions and special Jordan subalgebras
Ideals in power-associative algebras
Subspaces closed under multiplication by arbitrary elements from either side
Play a crucial role in the structure theory of power-associative algebras
Allow for the construction of quotient algebras
Nil ideals consist of nilpotent elements and are important for classification
Proper ideals in simple power-associative algebras must be zero
Representation theory
Representation theory studies algebras through their actions on vector spaces
Crucial for understanding the structure and properties of power-associative algebras
Bridges Non-associative Algebra with linear algebra and group theory
Linear representations
Homomorphisms from power-associative algebras to endomorphism algebras of vector spaces
Preserve power-associativity but not necessarily other algebraic properties
Regular representation uses the algebra itself as the representation space
Adjoint representation based on the left multiplication operators
Challenges in developing a comprehensive representation theory for non-associative algebras
Modules over power-associative algebras
Vector spaces equipped with an action of a power-associative algebra
Generalize the notion of modules over associative algebras
Right modules, left modules, and bimodules defined based on the action
Homomorphisms between modules preserve the algebra action
Challenges in defining tensor products and developing a full module theory