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PhyslibAlpha.AlgebraicFramework.JordanOrderUnit.JB.GeneratedByOne.CFC

Intrinsic continuous functional calculus for one JB observable

This file starts from the genuinely Jordan-theoretic spectral theorem in `GeneratedByOne.Spectrum`. In particular, its norm comparison is not imported from a Cstar realization: polynomial evaluation in the commutative associative algebra generated by `a` is isometric for the sup norm on the intrinsic real spectrum.

The remaining construction extends this isometry from polynomial functions to all continuous functions by Stone--Weierstrass and completeness.

The descended polynomial map

Completion from polynomial functions

Positive square roots

Absolute value and positive/negative parts

75 declarations

instance

The Jordan spectrum σ(a)\sigma(a) is compact

Let EE be a normed Jordan algebra and a∈Ea \in E. The Jordan spectrum of aa, denoted by σ(a)\sigma(a), is a compact topological space.

theorem

∥p(a)∥=∥p∥∞,σ(a)\|p(a)\| = \|p\|_{\infty, \sigma(a)} for polynomials in a JB algebra

Let EE be a nontrivial normed Jordan algebra that is also an archimedean order unit space (specifically a JB algebra). For any element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote its Jordan spectrum. For any polynomial p∈R[x]p \in \mathbb{R}[x], let p(a)p(a) denote the evaluation of pp at aa within the norm-closed Jordan subalgebra generated by 11 and aa. Then the norm of the element p(a)p(a) is equal to the supremum norm of pp viewed as a continuous function on the spectrum σ(a)\sigma(a): ∥p(a)∥=sup⁡λ∈σ(a)∣p(λ)∣.\|p(a)\| = \sup_{\lambda \in \sigma(a)} |p(\lambda)|. This equality establishes that polynomial evaluation is an isometry between the algebra of polynomials on σ(a)\sigma(a) and the polynomial core of the functional calculus in EE.

theorem

Density of Polynomial Functions on the Jordan Spectrum σ(a)\sigma(a)

Let aa be an element of a normed Jordan algebra EE. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa. The set of polynomial functions on σ(a)\sigma(a) is dense in the algebra C(σ(a),R)C(\sigma(a), \mathbb{R}) of continuous real-valued functions on the spectrum.

theorem

Every polynomial function on the Jordan spectrum σ(a)\sigma(a) has a polynomial representative p∈R[x]p \in \mathbb{R}[x]

Let EE be a normed Jordan algebra and a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa. For every function ff in the set of polynomial functions on σ(a)\sigma(a), there exists a polynomial p∈R[x]p \in \mathbb{R}[x] such that the continuous function induced by pp on σ(a)\sigma(a) is equal to ff.

definition

Polynomial representative of a polynomial function on the Jordan spectrum σ(a) \sigma(a)

For an element a a in a normed Jordan algebra E E and a function f f belonging to the algebra of polynomial functions on the Jordan spectrum σ(a)⊆R \sigma(a) \subseteq \mathbb{R} , this function selects a polynomial p∈R[x] p \in \mathbb{R}[x] such that the continuous function induced by p p on σ(a) \sigma(a) is equal to f f .

theorem

The polynomial representative of ff on σ(a)\sigma(a) induces ff

Let EE be a normed Jordan algebra and a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa. For any function ff in the algebra of polynomial functions on σ(a)\sigma(a), the continuous function on σ(a)\sigma(a) induced by the polynomial representative of ff is equal to ff.

theorem

p∣σ(a)=q∣σ(a)  ⟹  p(a)=q(a)p|_{\sigma(a)} = q|_{\sigma(a)} \implies p(a) = q(a) for Jordan observables

Let EE be a nontrivial normed Jordan algebra that is a partially ordered Archimedean additive monoid with a JB-order unit. For an element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote its Jordan spectrum. Given two polynomials p,q∈R[x]p, q \in \mathbb{R}[x], if their induced continuous functions on σ(a)\sigma(a) are equal (i.e., p(x)=q(x)p(x) = q(x) for all x∈σ(a)x \in \sigma(a)), then their evaluations at aa within the norm-closed subalgebra CJ(a)C_J(a) are also equal: p(a)=q(a)p(a) = q(a).

definition

Polynomial functional calculus linear map P(σ(a))→CJ(a)P(\sigma(a)) \to C_J(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)=J[a]‾C_J(a) = \overline{J[a]} be the norm-closed subalgebra generated by 11 and aa. Let P(σ(a))P(\sigma(a)) be the algebra of polynomial functions on the spectrum σ(a)\sigma(a). The linear map polynomialCfcLinearMap a:P(σ(a))→CJ(a)\text{polynomialCfcLinearMap } a : P(\sigma(a)) \to C_J(a) maps a function f∈P(σ(a))f \in P(\sigma(a)) to the element p(a)∈CJ(a)p(a) \in C_J(a), where p∈R[x]p \in \mathbb{R}[x] is any polynomial whose restriction to σ(a)\sigma(a) is ff.

theorem

The polynomial functional calculus map f↦f(a)f \mapsto f(a) is an isometry: ∥f(a)∥=∥f∥∞\|f(a)\| = \|f\|_\infty

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let σ(a)\sigma(a) be its Jordan spectrum and P(σ(a))P(\sigma(a)) be the algebra of polynomial functions on σ(a)\sigma(a). Let ϕa:P(σ(a))→CJ(a)\phi_a : P(\sigma(a)) \to C_J(a) be the polynomial functional calculus map that sends a function ff to the element f(a)f(a). Then for any f∈P(σ(a))f \in P(\sigma(a)), the norm of f(a)f(a) in the algebra is equal to the supremum norm of ff on the spectrum: ∥f(a)∥=∥f∥∞ \|f(a)\| = \|f\|_\infty

definition

Polynomial functional calculus linear isometry P(σ(a))→CJ(a)P(\sigma(a)) \to C_J(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)=J[a]‾C_J(a) = \overline{J[a]} be the norm-closed Jordan subalgebra generated by 11 and aa. Let P(σ(a))P(\sigma(a)) be the space of polynomial functions on σ(a)\sigma(a) equipped with the supremum norm. The map polynomialCfcLinearIsometry a:P(σ(a))→CJ(a)\text{polynomialCfcLinearIsometry } a : P(\sigma(a)) \to C_J(a) is a real linear isometry that sends a polynomial function f∈P(σ(a))f \in P(\sigma(a)) to the element p(a)∈CJ(a)p(a) \in C_J(a), where p∈R[x]p \in \mathbb{R}[x] is any polynomial whose restriction to σ(a)\sigma(a) is ff.

theorem

The polynomial functional calculus map is multiplicative: Φa(f⋅g)=Φa(f)⋅Φa(g)\Phi_a(f \cdot g) = \Phi_a(f) \cdot \Phi_a(g)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)\sigma(a) denote the Jordan spectrum of aa, and let P(σ(a))P(\sigma(a)) be the algebra of polynomial functions restricted to σ(a)\sigma(a). The polynomial functional calculus map Φa:P(σ(a))→CJ(a)\Phi_a : P(\sigma(a)) \to C_J(a) (mapping a function ff to the element f(a)f(a) in the closed subalgebra CJ(a)C_J(a)) is a homomorphism with respect to multiplication. That is, for any f,g∈P(σ(a))f, g \in P(\sigma(a)), the identity Φa(f⋅g)=Φa(f)⋅Φa(g)\Phi_a(f \cdot g) = \Phi_a(f) \cdot \Phi_a(g) holds, where the multiplication on the right is the Jordan product in EE (which is associative when restricted to CJ(a)C_J(a)).

definition

Continuous linear functional calculus C(σ(a),R)→CJ(a)C(\sigma(a), \mathbb{R}) \to C_J(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)=J[a]‾C_J(a) = \overline{J[a]} be the norm-closed Jordan subalgebra generated by 11 and aa. The continuous linear map C(σ(a),R)→CJ(a)C(\sigma(a), \mathbb{R}) \to C_J(a) is the canonical extension of the polynomial functional calculus to the space of continuous real-valued functions on the spectrum. It is constructed as the unique continuous extension of the linear isometry that maps a polynomial function p∣σ(a)p|_{\sigma(a)} to the element p(a)∈CJ(a)p(a) \in C_J(a), utilizing the fact that polynomial functions are dense in C(σ(a),R)C(\sigma(a), \mathbb{R}) by the Stone–Weierstrass theorem.

theorem

The continuous functional calculus coincides with the polynomial functional calculus for polynomial functions

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote its Jordan spectrum, and let CJ(a)C_J(a) denote the norm-closed Jordan subalgebra generated by 11 and aa. For any polynomial function f∈P(σ(a))f \in P(\sigma(a)) (where P(σ(a))P(\sigma(a)) is the space of polynomial functions restricted to the spectrum), the continuous linear functional calculus map and the polynomial functional calculus map agree on ff: jordanCfcLineara(f)=polynomialCfcLinearMapa(f)\text{jordanCfcLinear}_a(f) = \text{polynomialCfcLinearMap}_a(f) In other words, the continuous extension of the functional calculus is consistent with the initial definition for polynomial functions.

definition

Coordinate polynomial function on σ(a)\sigma(a)

For an element aa in a normed Jordan algebra EE, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} be its Jordan spectrum. The coordinate polynomial function is the function f:σ(a)→Rf: \sigma(a) \to \mathbb{R} defined by f(x)=xf(x) = x, regarded as an element of the algebra of polynomial functions on σ(a)\sigma(a). It is obtained by restricting the polynomial indeterminate XX to the set σ(a)\sigma(a).

theorem

The continuous Jordan functional calculus maps the coordinate function x↦xx \mapsto x to aa

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote its Jordan spectrum and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by the identity and aa. If f:σ(a)→Rf: \sigma(a) \to \mathbb{R} is the coordinate function defined by f(x)=xf(x) = x, then the continuous linear functional calculus map Ψ:C(σ(a),R)→CJ(a)\Psi: C(\sigma(a), \mathbb{R}) \to C_J(a) satisfies Ψ(f)=a\Psi(f) = a.

theorem

The continuous functional calculus map is an isometry: ∥f(a)∥=∥f∥∞\|f(a)\| = \|f\|_\infty

Let EE be a nontrivial normed Jordan algebra equipped with a JB-order unit structure. For any element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa and C(σ(a),R)C(\sigma(a), \mathbb{R}) denote the space of continuous real-valued functions on σ(a)\sigma(a). Let cfca:C(σ(a),R)→CJ(a)\text{cfc}_a : C(\sigma(a), \mathbb{R}) \to C_J(a) be the continuous functional calculus map which sends a function ff to the element f(a)f(a) in the closed Jordan subalgebra generated by 11 and aa. Then for any f∈C(σ(a),R)f \in C(\sigma(a), \mathbb{R}), the norm of the image is equal to the supremum norm of the function: ∥f(a)∥=∥f∥∞.\|f(a)\| = \|f\|_\infty. In other words, the continuous functional calculus map is a linear isometry.

definition

Continuous Jordan functional calculus linear isometry Ψa:C(σ(a),R)→CJ(a)\Psi_a : C(\sigma(a), \mathbb{R}) \to C_J(a)

Let EE be a nontrivial normed Jordan algebra equipped with a JB-order unit structure and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa and CJ(a)=J[a]‾C_J(a) = \overline{J[a]} denote the norm-closed Jordan subalgebra generated by the identity element 11 and aa. The continuous intrinsic Jordan functional calculus is the linear isometry Ψa:C(σ(a),R)→CJ(a)\Psi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) which maps a continuous real-valued function ff on the spectrum to the element f(a)f(a). As a linear isometry, it preserves the norm such that ∥Ψa(f)∥=∥f∥∞\|\Psi_a(f)\| = \|f\|_\infty for all f∈C(σ(a),R)f \in C(\sigma(a), \mathbb{R}).

theorem

Multiplicativity of the continuous Jordan functional calculus Φa(f⋅g)=Φa(f)⋅Φa(g)\Phi_a(f \cdot g) = \Phi_a(f) \cdot \Phi_a(g)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote its Jordan spectrum, and let Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) be the continuous linear functional calculus map, where CJ(a)C_J(a) is the norm-closed Jordan subalgebra generated by 11 and aa. For any continuous real-valued functions f,g∈C(σ(a),R)f, g \in C(\sigma(a), \mathbb{R}), the map Φa\Phi_a is multiplicative: Φa(f⋅g)=Φa(f)⋅Φa(g)\Phi_a(f \cdot g) = \Phi_a(f) \cdot \Phi_a(g) where f⋅gf \cdot g is the pointwise product of functions and the product on the right is the Jordan product in CJ(a)C_J(a).

theorem

jordanCfcLineara(1)=1\text{jordanCfcLinear}_a(1) = 1

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by the identity element 11 and aa. The continuous linear functional calculus map jordanCfcLineara:C(σ(a),R)→CJ(a)\text{jordanCfcLinear}_a : C(\sigma(a), \mathbb{R}) \to C_J(a) maps the constant function 11 on σ(a)\sigma(a) to the identity element 11 of CJ(a)C_J(a), i.e., jordanCfcLineara(1)=1.\text{jordanCfcLinear}_a(1) = 1.

definition

Continuous Jordan functional calculus as a unital algebra homomorphism C(σ(a),R)→CJ(a)C(\sigma(a), \mathbb{R}) \to C_J(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by 11 and aa. The continuous functional calculus for aa is the unital R\mathbb{R}-algebra homomorphism Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) which maps a continuous real-valued function ff on the spectrum to the element f(a)f(a) in CJ(a)C_J(a). This map is the unique continuous extension of the polynomial functional calculus p↦p(a)p \mapsto p(a).

theorem

The continuous Jordan functional calculus is an isometry

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by the identity 11 and aa. The continuous Jordan functional calculus R\mathbb{R}-algebra homomorphism Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) is an isometry. That is, for any continuous function f∈C(σ(a),R)f \in C(\sigma(a), \mathbb{R}), we have ∥Φa(f)∥=∥f∥∞\|\Phi_a(f)\| = \|f\|_\infty.

theorem

Φa(id)=a\Phi_a(\text{id}) = a for the continuous Jordan functional calculus

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by 11 and aa. The continuous Jordan functional calculus Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) maps the identity function id:σ(a)→R\text{id} : \sigma(a) \to \mathbb{R} (where id(x)=x\text{id}(x) = x) to the element aa. That is, Φa(id)=a\Phi_a(\text{id}) = a.

definition

Jordan continuous functional calculus f(a)f(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For an element a∈Ea \in E and a continuous real-valued function f∈C(σ(a),R)f \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a) of aa, the Jordan continuous functional calculus f(a)f(a) is the element of EE obtained by applying the unital R\mathbb{R}-algebra homomorphism Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) to ff and viewing the result as an element of the ambient algebra EE. Here CJ(a)C_J(a) denotes the norm-closed Jordan subalgebra generated by 11 and aa.

theorem

∥f(a)∥=∥f∥\|f(a)\| = \|f\| for the Jordan continuous functional calculus

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E and any continuous real-valued function f∈C(σ(a),R)f \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a), the norm of the element f(a)f(a) obtained through the Jordan continuous functional calculus is equal to the supremum norm of the function ff: ∥f(a)∥=∥f∥\|f(a)\| = \|f\|

theorem

Range of the Jordan Continuous Functional Calculus is Closed

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by the identity element 11 and aa. The range of the continuous functional calculus homomorphism Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) is a closed set.

definition

Canonical inclusion J[a]↪J[a]‾J[a] \hookrightarrow \overline{J[a]}

Let EE be a normed Jordan algebra and a∈Ea \in E. Let J[a]J[a] denote the Jordan subalgebra generated by the identity element 11 and the element aa, and let J[a]‾\overline{J[a]} denote its norm-closure. This definition is the canonical inclusion map from J[a]J[a] into J[a]‾\overline{J[a]}, treated as a linear map over R\mathbb{R}.

theorem

J[a]J[a] is dense in J[a]‾\overline{J[a]}

Let EE be a normed Jordan algebra and a∈Ea \in E. Let J[a]J[a] be the Jordan subalgebra generated by the identity element 11 and aa, and let J[a]‾\overline{J[a]} denote its norm-closure. The range of the canonical inclusion map J[a]↪J[a]‾J[a] \hookrightarrow \overline{J[a]} is dense in J[a]‾\overline{J[a]}.

theorem

The canonical inclusion of the Jordan power a[n]a^{[n]} into J[a]‾\overline{J[a]} equals ana^n

Let EE be a normed Jordan algebra and a∈Ea \in E. Let J[a]J[a] be the Jordan subalgebra generated by the identity 11 and aa, and let J[a]‾\overline{J[a]} be its norm-closure. Let ι:J[a]→J[a]‾\iota : J[a] \to \overline{J[a]} be the canonical inclusion map. For any n∈Nn \in \mathbb{N}, the image of the nn-th Jordan power a[n]a^{[n]} under ι\iota is equal to the nn-th power of aa in the commutative ring J[a]‾\overline{J[a]}, i.e., ι(a[n])=an.\iota(a^{[n]}) = a^n.

theorem

The Jordan power a[n]a^{[n]} lies in the range of the continuous functional calculus Φa\Phi_a

Let EE be a nontrivial normed Jordan algebra with a JB-order unit and a∈Ea \in E. Let J[a]‾\overline{J[a]} be the norm-closed Jordan subalgebra generated by 11 and aa, and let Φa:C(σ(a),R)→J[a]‾\Phi_a : C(\sigma(a), \mathbb{R}) \to \overline{J[a]} be the continuous functional calculus for aa. Then for every n∈Nn \in \mathbb{N}, the nn-th Jordan power a[n]a^{[n]}, when viewed as an element of J[a]‾\overline{J[a]}, lies in the range of Φa\Phi_a.

theorem

J[a]⊆range(Φa)J[a] \subseteq \text{range}(\Phi_a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any a∈Ea \in E, let J[a]J[a] be the Jordan subalgebra generated by the identity element 11 and aa, and let CJ(a)=J[a]‾C_J(a) = \overline{J[a]} be its norm-closure. Let Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) be the continuous functional calculus map, where σ(a)\sigma(a) is the Jordan spectrum of aa. For every x∈J[a]x \in J[a], its canonical inclusion in CJ(a)C_J(a) lies in the range of Φa\Phi_a.

theorem

Surjectivity of the Continuous Jordan Functional Calculus Φa\Phi_a onto CJ(a)C_J(a)

Let EE be a nontrivial normed Jordan algebra equipped with a JB-order unit. For any element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by 11 and aa. The continuous Jordan functional calculus, represented by the unital R\mathbb{R}-algebra homomorphism Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a), is surjective. That is, the range of Φa\Phi_a is the entirety of CJ(a)C_J(a).

theorem

The Range of the Continuous Jordan Functional Calculus is CJ(a)C_J(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit (formally, a partially ordered, Archimedean ordered additive monoid with monotone positive scalar multiplication). For any element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by the identity element 11 and aa. The continuous Jordan functional calculus is defined as the unital R\mathbb{R}-algebra homomorphism Φa:C(σ(a),R)→CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \to C_J(a) which maps a continuous real-valued function ff on the spectrum to an element f(a)∈CJ(a)f(a) \in C_J(a). This theorem states that the range of the homomorphism Φa\Phi_a is the entire subalgebra CJ(a)C_J(a).

definition

Jordan continuous functional calculus isomorphism C(σ(a),R)≅CJ(a)C(\sigma(a), \mathbb{R}) \cong C_J(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit, and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa, and let CJ(a)C_J(a) be the norm-closed Jordan subalgebra generated by 11 and aa. The continuous Jordan functional calculus is the unital R\mathbb{R}-algebra isomorphism Φa:C(σ(a),R)≅CJ(a) \Phi_a : C(\sigma(a), \mathbb{R}) \cong C_J(a) which identifies the algebra of continuous real-valued functions on the spectrum of aa with the closed associative subalgebra generated by aa. This map is obtained from the continuous functional calculus homomorphism by proving it is bijective (specifically, it is an isometry and its range is the entirety of CJ(a)C_J(a)).

theorem

The Continuous Jordan Functional Calculus is an Isometry: ∥Φa(f)∥=∥f∥\|\Phi_a(f)\| = \|f\|

Let EE be a nontrivial normed Jordan algebra that is a JB-algebra with an order unit. For any element a∈Ea \in E, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} be its Jordan spectrum, and let Φa:C(σ(a),R)≅CJ(a)\Phi_a : C(\sigma(a), \mathbb{R}) \cong C_J(a) be the continuous Jordan functional calculus isomorphism. For any continuous real-valued function ff on the spectrum of aa, the norm of the element Φa(f)\Phi_a(f) is equal to the supremum norm of ff, i.e., ∥Φa(f)∥=∥f∥.\|\Phi_a(f)\| = \|f\|.

theorem

The Jordan continuous functional calculus of the identity function is aa (coordinate law)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let id∈C(σ(a),R)\text{id} \in C(\sigma(a), \mathbb{R}) denote the restriction of the identity function x↦xx \mapsto x to the Jordan spectrum σ(a)\sigma(a). The Jordan continuous functional calculus applied to this identity function is aa itself, i.e., id(a)=a\text{id}(a) = a. This represents the coordinate law for the functional calculus.

theorem

(f+g)(a)=f(a)+g(a)(f + g)(a) = f(a) + g(a)

Let EE be a nontrivial normed Jordan algebra equipped with a JB-order unit. For any element a∈Ea \in E and any continuous real-valued functions f,g∈C(σ(a),R)f, g \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a), the Jordan continuous functional calculus satisfies (f+g)(a)=f(a)+g(a). (f + g)(a) = f(a) + g(a). Here, f(a)f(a) (represented as `jordanCfc a f`) denotes the result of applying the functional calculus to the element aa.

theorem

(f−g)(a)=f(a)−g(a)(f - g)(a) = f(a) - g(a) for Jordan continuous functional calculus

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E and any continuous real-valued functions f,g∈C(σ(a),R)f, g \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a) of aa, the Jordan continuous functional calculus preserves subtraction: (f−g)(a)=f(a)−g(a)(f - g)(a) = f(a) - g(a) where f(a)f(a) denotes the element of EE obtained by applying the functional calculus to the function ff at aa.

theorem

The Jordan continuous functional calculus of the zero function is zero

Let EE be a nontrivial normed Jordan algebra with a JB-order unit and let a∈Ea \in E. Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} be the Jordan spectrum of aa. The Jordan continuous functional calculus applied to the constant zero function 0∈C(σ(a),R)0 \in C(\sigma(a), \mathbb{R}) is equal to the zero element 0∈E0 \in E.

theorem

Multiplicativity of the Jordan Continuous Functional Calculus: (fg)(a)=f(a)g(a)(fg)(a) = f(a)g(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E and continuous real-valued functions f,g∈C(σ(a),R)f, g \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a), the Jordan continuous functional calculus satisfies (fg)(a)=f(a)g(a)(fg)(a) = f(a)g(a), where fgfg denotes the pointwise product of functions.

theorem

The Jordan continuous functional calculus of a constant function rr is r⋅1r \cdot 1

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E and any scalar r∈Rr \in \mathbb{R}, let f:σ(a)→Rf: \sigma(a) \to \mathbb{R} be the constant function defined by f(x)=rf(x) = r for all xx in the Jordan spectrum σ(a)\sigma(a). Then the Jordan continuous functional calculus of ff at aa satisfies f(a)=r⋅1f(a) = r \cdot 1, where 11 is the identity element of EE.

definition

Continuous square root function on the Jordan spectrum σ(a)\sigma(a)

Given an element aa of a normed Jordan algebra EE, this is the continuous function from the Jordan spectrum σ(a)⊆R\sigma(a) \subseteq \mathbb{R} to the real numbers defined by the map x↦xx \mapsto \sqrt{x}.

definition

Jordan square root a\sqrt{a} for a≥0a \geq 0

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For a non-negative element a∈Ea \in E (a≥0a \geq 0), the Jordan square root is the element of EE obtained by applying the Jordan continuous functional calculus to the square root function f(x)=xf(x) = \sqrt{x} defined on the Jordan spectrum σ(a)\sigma(a).

theorem

The square of the continuous square root function on σ(a)\sigma(a) is the identity map idσ(a)\text{id}_{\sigma(a)}

Let EE be a normed Jordan algebra (specifically a JB-algebra with an order unit) and let a∈Ea \in E be a positive element (a≥0a \ge 0). Let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote the Jordan spectrum of aa. Let f:σ(a)→Rf: \sigma(a) \to \mathbb{R} be the continuous square root function defined by f(x)=xf(x) = \sqrt{x}. Then the pointwise product of ff with itself satisfies f⋅f=idσ(a)f \cdot f = \text{id}_{\sigma(a)}, where idσ(a):σ(a)→R\text{id}_{\sigma(a)}: \sigma(a) \to \mathbb{R} is the identity function x↦xx \mapsto x restricted to the spectrum.

theorem

a⋅a=a\sqrt{a} \cdot \sqrt{a} = a for a≥0a \ge 0

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any non-negative element a∈Ea \in E (a≥0a \ge 0), let a\sqrt{a} denote the Jordan square root of aa (the element obtained by applying the Jordan continuous functional calculus to the function f(x)=xf(x) = \sqrt{x} on the spectrum of aa). Then the Jordan product of a\sqrt{a} with itself satisfies a⋅a=a\sqrt{a} \cdot \sqrt{a} = a.

theorem

a≥0  ⟹  a≥0a \ge 0 \implies \sqrt{a} \ge 0 in JB-algebras

Let EE be a nontrivial normed Jordan algebra equipped with a JB-order unit (a JB-algebra). For any non-negative element a∈Ea \in E (where a≥0a \ge 0), its Jordan square root a\sqrt{a}, obtained via the Jordan continuous functional calculus for the function f(x)=xf(x) = \sqrt{x}, is also non-negative, i.e., 0≤a0 \le \sqrt{a}.

theorem

f=g2  ⟹  f(a)≥0f = g^2 \implies f(a) \ge 0 in Jordan Continuous Functional Calculus

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E and any continuous real-valued functions f,g∈C(σ(a),R)f, g \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a), if f=g2f = g^2, then the element f(a)f(a) obtained via the Jordan continuous functional calculus is non-negative, i.e., f(a)≥0f(a) \ge 0.

theorem

Positivity of the Jordan continuous functional calculus: f≥0  ⟹  f(a)≥0f \ge 0 \implies f(a) \ge 0

Let EE be a nontrivial normed Jordan algebra equipped with a JB-order unit. For any element a∈Ea \in E and any continuous real-valued function f∈C(σ(a),R)f \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a) of aa, if ff is pointwise nonnegative (i.e., f(x)≥0f(x) \ge 0 for all x∈σ(a)x \in \sigma(a)), then the element f(a)f(a) obtained via the Jordan continuous functional calculus is also nonnegative in EE, so that 0≤f(a)0 \le f(a).

theorem

The Jordan continuous functional calculus is monotone: f≤g  ⟹  f(a)≤g(a)f \le g \implies f(a) \le g(a)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E and any continuous real-valued functions f,g∈C(σ(a),R)f, g \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a), if f≤gf \le g pointwise (i.e., f(x)≤g(x)f(x) \le g(x) for all x∈σ(a)x \in \sigma(a)), then f(a)≤g(a)f(a) \le g(a) holds in EE, where f(a)f(a) and g(a)g(a) denote the elements obtained via the Jordan continuous functional calculus.

theorem

0≤f(a)  ⟺  ∀x,0≤f(x)0 \leq f(a) \iff \forall x, 0 \leq f(x) for the Jordan continuous functional calculus

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E and any continuous real-valued function f∈C(σ(a),R)f \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a), the element f(a)f(a) obtained via the Jordan continuous functional calculus is non-negative (0≤f(a)0 \leq f(a)) if and only if f(x)≥0f(x) \geq 0 for all x∈σ(a)x \in \sigma(a).

theorem

f(a)≤g(a)  ⟺  f≤gf(a) \leq g(a) \iff f \leq g for the Jordan continuous functional calculus

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For an element a∈Ea \in E and any two continuous real-valued functions f,g∈C(σ(a),R)f, g \in C(\sigma(a), \mathbb{R}) defined on the Jordan spectrum σ(a)\sigma(a), the inequality f(a)≤g(a)f(a) \leq g(a) holds in EE if and only if f(x)≤g(x)f(x) \leq g(x) for all x∈σ(a)x \in \sigma(a).

theorem

b∈CJ(a),b≥0,b2=a  ⟹  b=ab \in C_J(a), b \geq 0, b^2 = a \implies b = \sqrt{a}

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any non-negative element a∈Ea \in E (a≥0a \geq 0), let CJ(a)C_J(a) be the norm-closure of the subalgebra generated by 11 and aa. If there exists an element b∈CJ(a)b \in C_J(a) such that b≥0b \geq 0 and b2=ab^2 = a, then bb is equal to the Jordan square root a\sqrt{a} obtained via the continuous functional calculus.

definition

Absolute value function on the Jordan spectrum σ(a)\sigma(a)

For an element aa in a normed Jordan algebra EE, this function is the continuous map from the Jordan spectrum σ(a)⊆R\sigma(a) \subseteq \mathbb{R} to R\mathbb{R} defined by the absolute value x↦∣x∣x \mapsto |x| for all x∈σ(a)x \in \sigma(a).

definition

Intrinsic absolute value ∣a∣|a| of a JB observable

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For an element a∈Ea \in E, the intrinsic absolute value ∣a∣|a| is defined by applying the Jordan continuous functional calculus to the absolute value function f:σ(a)→Rf: \sigma(a) \to \mathbb{R}, given by f(x)=∣x∣f(x) = |x|, where σ(a)\sigma(a) is the Jordan spectrum of aa.

theorem

∣a∣2=a2|a|^2 = a^2 for a JB observable aa

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let ∣a∣|a| denote its intrinsic absolute value defined via the Jordan continuous functional calculus. Then the Jordan product of the absolute value with itself is equal to the Jordan product of aa with itself: ∣a∣2=a2|a|^2 = a^2

theorem

The intrinsic absolute value ∣a∣|a| is non-negative (0≤∣a∣0 \le |a|) for JB observables

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, its intrinsic absolute value ∣a∣|a| (defined by applying the Jordan continuous functional calculus to the absolute value function f(x)=∣x∣f(x) = |x| on the spectrum σ(a)\sigma(a)) is non-negative, that is, 0≤∣a∣0 \le |a|.

theorem

∣a∣=0  ⟺  a=0|a| = 0 \iff a = 0

Let EE be a nontrivial normed Jordan algebra equipped with a JB-order unit. For any element a∈Ea \in E, the intrinsic absolute value ∣a∣|a| (defined via the Jordan continuous functional calculus applied to the function f(x)=∣x∣f(x) = |x|) vanishes if and only if aa is the zero element. That is, ∣a∣=0  ⟺  a=0|a| = 0 \iff a = 0.

theorem

a≥0  ⟹  ∣a∣=aa \ge 0 \implies |a| = a

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E such that a≥0a \ge 0, its intrinsic absolute value satisfies ∣a∣=a|a| = a.

theorem

∣a∣=a  ⟺  0≤a|a| = a \iff 0 \le a

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, the intrinsic absolute value ∣a∣|a| satisfies ∣a∣=a|a| = a if and only if 0≤a0 \le a.

definition

Positive part function on the Jordan spectrum σ(a)\sigma(a)

For an element a a in a normed Jordan algebra E E , this function represents the continuous real-valued function on the Jordan spectrum σ(a) \sigma(a) defined by x↦max⁡(x,0) x \mapsto \max(x, 0) . This is the positive-part function restricted to the set of values in the spectrum.

definition

Negative part function on the Jordan spectrum σ(a)\sigma(a)

For an element aa in a normed Jordan algebra EE, let σ(a)⊆R\sigma(a) \subseteq \mathbb{R} denote its Jordan spectrum. The definition `jordanSpectrumNegPart` is the continuous real-valued function f∈C(σ(a),R)f \in C(\sigma(a), \mathbb{R}) that maps each x∈σ(a)x \in \sigma(a) to its negative part, defined by f(x)=max⁡(−x,0)f(x) = \max(-x, 0).

definition

Positive part a+a^+ of a Jordan observable aa

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For an element a∈Ea \in E, the positive part is defined as the element f(a)∈Ef(a) \in E obtained by applying the Jordan continuous functional calculus to the continuous function f:σ(a)→Rf: \sigma(a) \to \mathbb{R} given by f(x)=max⁡(x,0)f(x) = \max(x, 0), where σ(a)\sigma(a) denotes the Jordan spectrum of aa.

definition

Negative part a−a^- of a Jordan observable aa

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For an element a∈Ea \in E, the negative part of aa is defined as the element a−=f(a)∈Ea^- = f(a) \in E obtained by applying the Jordan continuous functional calculus to aa and the continuous function f:σ(a)→Rf: \sigma(a) \to \mathbb{R} defined on the Jordan spectrum σ(a)\sigma(a) by f(x)=max⁡(−x,0)f(x) = \max(-x, 0).

theorem

The positive part a+a^+ of a Jordan observable is non-negative (0≤a+0 \leq a^+)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, its positive part a+a^+ (defined as the element obtained by applying the Jordan continuous functional calculus to aa for the function f(x)=max⁡(x,0)f(x) = \max(x, 0)) satisfies 0≤a+0 \leq a^+.

theorem

The negative part a−a^- is non-negative (0≤a−0 \le a^-)

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, its negative part a−a^- is non-negative, satisfying 0≤a−0 \le a^-. The negative part a−a^- is defined as the element obtained by applying the Jordan continuous functional calculus to aa for the continuous function f(x)=max⁡(−x,0)f(x) = \max(-x, 0).

theorem

a+=aa^+ = a for a≥0a \ge 0

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, if 0≤a0 \le a, then its positive part a+a^+ is equal to aa. Here, the positive part a+a^+ is defined as the element obtained by applying the Jordan continuous functional calculus to aa for the function f(x)=max⁡(x,0)f(x) = \max(x, 0).

theorem

The negative part a−a^- of a positive observable a≥0a \geq 0 is 00

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E such that 0≤a0 \leq a, its negative part a−a^- (defined via the Jordan continuous functional calculus for the function f(x)=max⁡(−x,0)f(x) = \max(-x, 0)) is equal to 00.

theorem

a=a+−a−a = a^+ - a^- for a Jordan observable aa

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let a+a^+ and a−a^- denote the positive and negative parts of aa, respectively. Then, the element aa can be reconstructed from these parts as a=a+−a−a = a^+ - a^-.

theorem

a−=0  ⟺  0≤aa^- = 0 \iff 0 \le a for a Jordan observable aa

Let EE be a nontrivial normed Jordan algebra equipped with an Archimedean order unit. For any element a∈Ea \in E, let a−a^- denote its negative part, defined by applying the Jordan continuous functional calculus to the function x↦max⁡(−x,0)x \mapsto \max(-x, 0). Then a−=0a^- = 0 if and only if 0≤a0 \le a.

theorem

a+=0a^+ = 0 if and only if a≤0a \le 0 for Jordan observables

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let a+a^+ denote its positive part, defined via the continuous functional calculus as the element f(a)f(a) where f(x)=max⁡(x,0)f(x) = \max(x, 0). Then a+=0a^+ = 0 if and only if a≤0a \leq 0.

theorem

∣a∣=a++a−|a| = a^+ + a^- for a Jordan observable aa

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let ∣a∣|a| denote the intrinsic absolute value of aa, a+a^+ denote its positive part, and a−a^- denote its negative part. Then the absolute value is the sum of the positive and negative parts: ∣a∣=a++a−.|a| = a^+ + a^-.

theorem

a+≤∣a∣a^+ \le |a| for a Jordan observable aa

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, the positive part a+a^+ (defined via the continuous functional calculus as the element corresponding to the function f(x)=max⁡(x,0)f(x) = \max(x, 0)) is bounded by the intrinsic absolute value ∣a∣|a| (defined as the element corresponding to f(x)=∣x∣f(x) = |x|). That is, a+≤∣a∣a^+ \le |a|.

theorem

a−≤∣a∣a^- \le |a| for a Jordan observable aa

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, the negative part a−a^- is less than or equal to the intrinsic absolute value ∣a∣|a|, that is, a−≤∣a∣.a^- \le |a|.

theorem

a≤∣a∣a \le |a| for a JB observable

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, it holds that a≤∣a∣a \le |a|, where ∣a∣|a| is the intrinsic absolute value of aa defined by the Jordan continuous functional calculus.

theorem

−a≤∣a∣-a \le |a| for a JB observable

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, it holds that −a≤∣a∣,-a \le |a|, where ∣a∣|a| denotes the intrinsic absolute value of aa defined via the Jordan continuous functional calculus.

theorem

Jordan-orthogonality of a+a^+ and a−a^-

Let EE be a nontrivial normed Jordan algebra with a JB-order unit. For any element a∈Ea \in E, let a+a^+ be its positive part and a−a^- be its negative part. Then a+a^+ and a−a^- are Jordan-orthogonal, meaning their Jordan product satisfies a+∘a−=0a^+ \circ a^- = 0.