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In mathematics, a
Lie algebra In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an operation called the Lie bracket, an alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow \mathfrak g, that satisfies the Jacobi ident ...
has been generalized in several ways.


Graded Lie algebra and Lie superalgebra

A graded Lie algebra is a Lie algebra with grading. When the grading is \mathbb/2, it is also known as a Lie superalgebra.


Lie-isotopic algebra

A Lie-isotopic algebra is a generalization of Lie algebras proposed by physicist R. M. Santilli in 1978.


Definition

Recall that a finite-dimensional
Lie algebra In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an operation called the Lie bracket, an alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow \mathfrak g, that satisfies the Jacobi ident ...
L with generators X_1, X_2, ..., X_n and commutation rules : _i X_j= X_i X_j - X_j X_i = C_^k X_k, can be defined (particularly in physics) as the totally anti-symmetric algebra A(L)^- attached to the universal enveloping associative algebra A(L)=\ equipped with the associative product X_i \times X_j over a numeric field F with multiplicative unit 1. Consider now the axiom-preserving lifting of A(L) into the form A^*(L^*)=\, called universal enveloping isoassociative algebra, with isoproduct :X_i\times X_j = X_i T^* X_j, verifying the isoassociative law :X_i\times (X_j \times X_k) = X_i\times (X_j \times X_k) and multiplicative isounit :1^* = 1/T*, 1^* \times X_k = X_k \times 1^* = X_k \forall X_k in A^*(L^*) where T^*, called the isotopic element, is not necessarily an element of A(L) which is solely restricted by the condition of being positive-definite, T^* > 0 , but otherwise having any desired dependence on local variables, and the products X_i T^*, T^* X_j, etc. are conventional associative products in A(L). Then a Lie-isotopic algebra L^* can be defined as the totally antisymmetric algebra attached to the enveloping isoassociative algebra. L^* = A^*(L^*)^- with isocommutation rules : _i, X_j* = X_i \times X_j - X_j \times X_i = X_i T^* X_j - X_j T^* X_i = C_^ X_k. It is evident that: 1) The isoproduct and the isounit coincide at the abstract level with the conventional product and; 2) The isocommutators _i, X_j* verify Lie's axioms; 3) In view of the infinitely possible isotopic elements T^* (as numbers, functions, matrices, operators, etc.), any given Lie algebra L admits an infinite class of isotopes; 4) Lie-isotopic algebras are called regular whenever C_^ = C_^, and irregular whenever C_^ \ne C_^. 5) All regular Lie-isotope L^* are evidently isomorphic to L. However, the relationship between irregular isotopes L^* and L does not appear to have been studied to date (Jan. 20, 2024). An illustration of the applications cf Lie-isotopic algebras in physics is given by the isotopes SU^*(2) of the SU(2)-spin symmetry whose fundamental representation on a Hilbert space H over the field of complex numbers C can be obtained via the nonunitary transformation of the fundamental reopreserntation of SU(2) (Pauli matrices) : \sigma^*_k = U \sigma_k U^\dagger, : U U^\dagger = I ^* = Diag. (\lambda^, \lambda), Det 1^* = 1, : \sigma^*_1= \left(\! \begin 0& \lambda\\ \lambda^& 0 \end \!\right), \sigma^*_2 = \left(\! \begin 0& -i\! \lambda\\ i\! \lambda^& 0 \end \!\right), \sigma^*_3 = \left(\! \begin \lambda^& 0\\ 0& -\lambda \end \!\right ), providing an explicit and concrete realization of Bohm's hidden variables \lambda, which is 'hidden' in the abstract axiom of associativity and allows an exact representation of the Deuteron magnetic moment.


Lie n-algebra


Quasi-Lie algebra

A quasi-Lie algebra in
abstract algebra In mathematics, more specifically algebra, abstract algebra or modern algebra is the study of algebraic structures, which are set (mathematics), sets with specific operation (mathematics), operations acting on their elements. Algebraic structur ...
is just like a
Lie algebra In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an operation called the Lie bracket, an alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow \mathfrak g, that satisfies the Jacobi ident ...
, but with the usual
axiom An axiom, postulate, or assumption is a statement that is taken to be true, to serve as a premise or starting point for further reasoning and arguments. The word comes from the Ancient Greek word (), meaning 'that which is thought worthy or ...
: ,x0 replaced by : ,y- ,x/math> (anti-symmetry). In characteristic other than 2, these are equivalent (in the presence of
bilinearity In mathematics, a bilinear map is a function combining elements of two vector spaces to yield an element of a third vector space, and is linear in each of its arguments. Matrix multiplication is an example. A bilinear map can also be defined for ...
), so this distinction doesn't arise when considering real or complex Lie algebras. It can however become important, when considering ''Lie algebras'' over the integers. In a quasi-Lie algebra, :2 ,x0. Therefore, the bracket of any element with itself is 2-torsion, if it does not actually vanish. See also:
Whitehead product In mathematics, the Whitehead product is a graded quasi-Lie algebra structure on the homotopy groups of a space. It was defined by J. H. C. Whitehead in . The relevant MSC code is: 55Q15, Whitehead products and generalizations. Definition G ...
.


References

*


Further reading

*https://www.researchgate.net/publication/250736074_Some_remarks_on_Lie-isotopic_lifting_of_Minkowski_metric *https://onlinelibrary.wiley.com/doi/abs/10.1002/(SICI)1099-1476(19961125)19:17%3C1349::AID-MMA823%3E3.0.CO;2-B Lie algebras {{algebra-stub