symmetric monoidal (∞,1)-category of spectra
theory (physics), model (physics)
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A Jordan-Lie-Banach algebra (or JLB-algebra for short) is a topological algebra that behaves like a Poisson algebra, only that the commutative product is not required to form an associative algebra, but just a Jordan algebra. Hence a JLB-algebra is a nonassociative Poisson algebra with topology.
JLB-algebras are the outcome of quantization of Poisson algebras. Often that outcome is regarded to be a non-commutative but associative C-star-algebra. But any such induces a JLB-algebra by letting the Jordan product be the symmetrized product and the Lie bracket the commutator. There is a condition relating the associator of the JLB-algebra to the Lie bracket, that characterizes those JLB-algebras that come from non-commutative associative algebras, and in the usual definition of JLB-algebra this condition is required. In that case JLB-algebras are effectively the same as -algebras, the only difference being that the single assocative product is explcitly regarded as inducing the two products of a non-associative Poisson algebra.
A careful definition is in section 1.1 of
A brief remark is on p. 80 of