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Functional analysis Definition

Jordan operator algebra

Builds on Hilbert spaceSelf-adjoint operatorJordan algebraSpecial Jordan algebra

Definition

Let HH be a complex Hilbert space. Let B(H)saB(H)_{\mathrm{sa}} be the real vector space of bounded self-adjoint operators on HH, with the operator norm ∥⋅∥\norm{\cdot}. For a,b∈B(H)saa, b \in B(H)_{\mathrm{sa}} put a∘b=12(ab+ba)a \circ b = \frac{1}{2}(ab + ba). A Jordan operator algebra, or JC-algebra, on HH is a real linear subspace A⊆B(H)saA \subseteq B(H)_{\mathrm{sa}} such that:

  1. a∘b∈Aa \circ b \in A for all a,b∈Aa, b \in A;
  2. AA is closed in the norm topology.

Remarks

Each JC-algebra is a special Jordan algebra, as a Jordan subalgebra of B(H)+B(H)^+. Clause 1 is equivalent to a2∈Aa^2 \in A for all a∈Aa \in A, since a∘b=12((a+b)2−a2−b2)a \circ b = \frac{1}{2}((a + b)^2 - a^2 - b^2).

Example: H=ℂnH = \C^n and AA the real symmetric n×nn \times n matrices. For symmetric aa and bb, (ab+ba)T=ba+ab(ab + ba)^T = ba + ab, so clause 1 holds, and AA is closed because it is finite-dimensional.

Non-example: for H=ℂ2H = \C^2, the real span of the Pauli matrices σx=(0110)\sigma_x = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix} and σz=(100−1)\sigma_z = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix} fails clause 1. Indeed σx∘σx=I\sigma_x \circ \sigma_x = I, and II is not a combination of σx\sigma_x and σz\sigma_z.

A JC-algebra that is closed in the weak operator topology is called a JW-algebra.

Reading path

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  1. Hilbert space concept
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  3. Self-adjoint operator concept
  4. Special Jordan algebra concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Jordan_operator_algebra
About this page
TagQZH32DH8SX
URIm2://QZH32DH8SX
Kinddefinition
WritingW0 stub
MSC46L70, 17C65
DefinesJordan operator algebra
UsesHilbert space, Self-adjoint operator, Jordan algebra, Special Jordan algebra
Changed3 November 2026

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